1School of Mechanical and Mining Engineering, The University of Queensland, Brisbane, Queensland 4072, Australia.
2Centre for Future Materials, University of Southern Queensland, Springfield Central, Queensland 4300, Australia.
3Centre for Microscopy and Microanalysis, The University of Queensland, Brisbane, Queensland 4072, Australia.
#Authors contributed equally.
© The Author(s) 2021. Open Access This article is licensed under a Creative Commons Attribution 4.0 International License (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, sharing, adaptation, distribution and reproduction in any medium or format, for any purpose, even commercially, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.
Conducting polymer-based thermoelectric materials are considered the most promising candidates for applying to wearable thermoelectric devices because of their high electrical conductivities, flexibility, stability, and low-toxicity features. Therefore, a timely review is needed to comprehensively overview their most recent progress in the last few years, considering the rapid development of thermoelectric conducting polymers. In this work, we carefully summarize recent advances in thermoelectric conducting polymers from aspects of their mechanisms, synthesis, micro/nanostructures, mechanical/thermoelectric properties, and related functional devices. A few state-of-the-art thermoelectric conducting polymers, including poly(3,4-ethylenedioxythiophene)poly(styrenesulfonate), poly(3-hexylthiophene), polyaniline, and polypyrrole, are highlighted in detail. In the end, we point out the challenges, controversies, and outlooks of conducting polymers for future thermoelectric applications.
Thermoelectric, conducting polymer, synthesis, performance, device
With the depletion of indispensable non-renewable energy sources such as petroleum and natural gas, extensive investigations focus on sustainable technologies for harvesting green energy from wind, solar, bioenergy, and waste heat. Thermoelectric (TE) materials and devices, with the capability for direct conversion between heat and electricity, show great potentials as sustainable and green technologies[2-6]. In order to evaluate the TE potential of a material, a dimensionless figure of merit ZT is defined by
Since the 1950s, early TE materials such as Bi2Te3[11,12] have been widely used in various fields, but their performance is not ideal with a ZT of up to one unit. With the rapid development, nowadays many thermoelectric materials, such as PbTe, Pr2CoFeO6, SrTiO3, SnTe[17,18], Cu2Se, SnSe[20-24], and GeTe[25-28], have exhibited high ZTs of > 2, by using the rational electronic band structure design for boosting S2σ, and/or by using micro/nanostructure manipulations for achieving low κ. In addition to conventional bulk TE materials, conducting polymer-based thermoelectric materials is increasingly popular and shows high flexibility and promising TE performance. These conducting polymer-based thermoelectric materials target flexible TE generators (F-TEGs) with broad practical applications such as charging wearable and portable electronics. As can be seen from Figure 1A[10,29], F-TEGs tend to serve implantable and wearable electronic devices such as smart glasses, smart watches, and trackers, which only need low energy demand, as suggested in Figure 1B. The increase in demand for lightweight, high-performance, and inexpensive products is driving the growth of the global conductive polymer market. Specifically, the conductive polymer industry was pegged at $3.46 billion in 2020 and is projected to reach $5.76 billion with a compound annual growth rate of 8.3% from 2021 to 2027. Therefore, high-performance, low-toxic, and high-stability F-TEGs are the most promising candidates to meet the demand of the future electronic market[33-35]. Similar to conventional TE devices, the structure of F-TEGs can be described as the combination of several pairs of p- and n-type TE materials, as shown in Figure 1C[1,36-38].
Figure 1. (A) Wearable and implantable devices, clothing, and objects. Reproduced with permission. Copyright 2019 Wiley. Reproduced with permission. Copyright 2020 Cambridge University Press. (B) Heat dissipated from various parts of the human body. Copyright 2020 Wiley. (C) Schematic diagram for the assembly of thermoelectric devices. Copyright 2020 ACS publications. (D) Comparison of S2σ values for the state of-the-art polypyrrole (PPy)[39-43], polyaniline (PANI)[44-48], poly(3-hexylthiophene) (P3HT)[49-54], and poly(3,4-ethylenedioxythiophene)poly(styrenesulfonate) (PEDOT: PSS)[55-59].
In recent years, conducting polymers have exhibited promising TE performance, benefited from many advanced strategies such as doping, pre- and post-treatments, and hybridization. Figure 1D summarizes S2σ values of the state-of-the-art conducting polymers developed in recent 5 years, including polypyrrole (PPy)[39-43], polyaniline (PANI)[44-48], poly(3-hexylthiophene) (P3HT)[49-54], and poly(3,4-ethylenedioxythiophene)poly(styrenesulfonate) (PEDOT: PSS)[55-59], which possess the high possibility to be applied in wearable F-TEGs. Considering the rapid development of conducting polymers that target F-TEGs, a timely review is needed to overview their most recent progress comprehensively. We carefully summarize the advances in state-of-the-art conducting polymers from the aspects of mechanisms, synthesis, micro/nanostructures, mechanical and TE properties, and F-TEGs. Particularly, the state-of-the-art systems, including PEDOT: PSS, P3HT, PANI, and PPy, are detailed discussed. In the end, we point out the challenges, controversies, and outlooks of conducting polymers for future TE applications.
Based on the Seebeck effect[62-66], TEGs can generate electricity by utilizing temperature difference ΔT. Therefore, charge transport is a vital part of the TE conversion. For polymer-based TE materials, the charge transport mechanism is different from conventional inorganic TE materials. In conducting polymers, the structure of the π-conjugated skeleton is closely relevant to charge transport. Figure 2A illustrates the valence band (π orbital), the conduction band (π* orbital), and the band gap of trans-polyacetylene, one kind of typical conducting polymers. Due to the weak interaction force between organic molecules, the thermal drive causes the dynamic disorder of the molecules, which directly affects the mobility of carriers. Such a band structure is similar to conventional inorganic TE materials, where the charge transport is determined by conduction/valence bands and band-gap value. Therefore, rational doping can effectively alter the band structure and, in turn, significantly improve the charge transport of conducting polymers.
Figure 2. (A) Valence band π and conduction band π* orbital energy diagram of trans-polyacetylene. Reproduced with permission. Copyright 2012 Royal Society of Chemistry. (B) Potential energy diagram of charge transfer reaction in conducting polymers. Reproduced with permission. Copyright 2007 CRC Press. (C) Schematic diagram of the electron transport path in conducting polymers. Reproduced with permission. Copyright 2006 Oxford University Press. (D) Schematic diagram of the formation of polarons in conducting polymers under the influence of positive charges. Reproduced with permission. Copyright 2007 CRC Press.
Because the charge transport mechanism is complicated in organic molecules, a few different models have been developed to investigate charge transport behaviors. Bimolecular reaction (Marcus model) is one of the typical models. According to this model, the basic reaction can be described as D- + A → D + A-. Figure 2B describes the energy change based on the reaction by the Marcus model, where ΔG# is the energy barrier and related to the charge transfer integral (t). In this model, ΔG# = (λ-2t)2(4λ)-1 = λ/4 - t (t < λ), and λ = f (qR-qP)2/2. Here, f is the oscillation intensity, and qR and qP are coordinate reactants and products. Marcus theory can be linked to charge transfer speed and carrier mobility µ. According to the relationship between λ and 2t, the charge transfer can be divided into band-like and hopping models. In the band-like transport model, carriers move freely in the energy band. If there is no external electric field, carriers only have free thermal motion, while if an electric field is applied, carriers move under the influence of the electric field. Figure 2C shows the carrier transport path with or without an external electric field. With increasing the temperature, σ and μ decrease. This model is suitable for conducting polymers with high intrinsic σ and materials with low doping concentration. In terms of the hopping model, conducting polymers are difficult to form a high-regularity structure like crystals; therefore, the localized charge in amorphous organics moves in a hopping manner. In solid materials, the localized charge appears “self-trapped”, which causes obvious displacement of the surrounding atoms. This charge forms a polaron with the polarized cloud induced around. Among them, the polarization effect of conducting polymers mainly comes from the polarization of the surrounding π electron cloud, as shown in Figure 2D.
As mentioned above, overloaded carriers move driven by the temperature field so that S can be defined as the entropy change caused by the thermally excited carrier transport. Besides, the core mechanism of the TE conversion reveals the effect of carrier transport related to σ and S. The conversion mechanism also indicates that σ and S are mutually restrictive; they are both directly affected by the carrier concentration n (np for the materials with holes as major carriers, and ne for the materials with electrons as major carriers). Interestingly, S decreases as n increases, and σ is the opposite. At the same time, the electronic thermal conductivity κe is directly related to n. For conducting polymers, peaks of these three parameters roughly appear in the interval of n of 1019-1021 cm-3. The current challenge of explaining the charge transport mechanism of conducting polymers is that S and σ are influenced by different transport mechanisms, although researchers have tried to develop different transport models. To date, the developed models include (1) The nearest-neighbor model describes the transport of electronic charges from Site A to Site B, with other charges filling Site A simultaneously, which is used when the conductive polymers are heavily used doped. Particularly, under thermal excitation, this model is generally used to explain the carrier transport behaviors. However, the apparent shortcoming is low accuracy as well as the sites distance limitation. (2) Variable-range hopping model is used to describe localized states distributed in a large energy band, which determines σ without neglecting the energy-dependent term. Generally, this model can be adapted in conductive polymer-doped situations. (3) Mobility edge model is suitable for describing charges excited into delocalized states. Compared with the hopping model, the mobility edge model matches the conductive polymers with higher σ[73-75]. (4) Transport edge model is suitable for some advanced conductive polymers with a higher σ similar to metals, which are more able to follow S ∝ σ 1/4 empirical power law. (5) Heterogeneous media model is suitable for describing disordered regions of conductive polymer with poor σ. However, conductive polymers are not completely disorders or crystalline; instead, the small crystalline domains range from 10 to 50 nm, connect according to disordered regions and connect by several extended polymer chains. Hence, the model is effective when the conductive polymer has both high and poor σ sections in series.
κ is an inherent property of most materials. Usually, κ is calculated using Fourier's law[77,78]. The κ value is affected by both phonons and electrons because κ is composed of κe (the influence of electrons) and κl (the influence of phonon)[10,79]. κe is the heat transfer affected by electron diffusion, which has a positive correlation with σ. while, κl does not influence σ; instead, κl is related to the vibration of the lattice. Generally, a hierarchical structure with multi-dimensional structural imperfections can sharply decrease κl[80,81]. Generally, conductive polymers are typical low-crystallinity materials with entanglement, chain ends, voids, and impurities as intrinsic defects. Entanglement is one of the most common defects mainly found in thick fibers, leading to interchain transport instead of intrachain transport and, in turn, altering the phonon transport behavior. Chain ends shorten the effective heat transport because the covalent bonds of the polymer chain dominate the κ. Voids influence the effective κ with its morphology, volume, and pore size. Among these, the pore size has the most significant influence on phonon transport. As for impurities, their volume fraction, interface thermal resistance, particle size, and aspect ratio also affect the phonon transport behavior. Therefore, phonon transfer plays a crucial role in κ of polymers.
Figure 3A compares temperature-dependent κ of conducting polymers with different structures, including disordered polymer, organic crystal, Poly(ethylene glycol)-block-poly(propylene glycol)-blockpoly(ethylene glycol) triblock copolymer (PEPG) treated PEDOT: PSS with high crystallinity and low crystallinity. Previous works tried to explain the relationship between κ of insulating crystal change and thermodynamics. Peierls first introduced the theory by conservation of momentum. In a conventional process, phonons exhibit momentum conservation. However, in the Umklapp process, momentum is not conserved, and the conservation needs to consider the changes brought by the movement of the entire crystal. As shown in Figure 3B, in the theoretical process, Phonon-3 can be superimposed by Phonon-1 and Phonon-2. In the Umklapp process, because of the discrete nature of the atomic lattice, there is a minimum phonon vibration wavelength that represents the maximum allowable vector wave. The vector wave generated by the combination of two phonons is greater than this allowable value. In this situation, the direction of the phonons can be deflected, and the lattice vector G needs to be given to balance the differences between the theoretical vector sum and the actual vector sum.
Figure 3. (A) Temperature-dependent κ of conducting polymers with various structures. Reproduced with permission Copyright Royal Society of Chemistry; (B) schematic diagram of phonon transport and scattering vector. Reproduced with permission. Copyright ProQuest Dissertations Publishing. Phonon movement in (C) amorphous polymer, (D) crystalline materials, and (E) hybrid materials, respectively. Reproduced with permission. Copyright ELSEVIER.
Phonon transport in pure polymer composites is shown in Figure 3C. Phonon transport between the same types of atoms is almost directly transported without scattering. However, phonons can be scattered if the atoms are different in type, or there are defects in the microstructure or impurities. Polymer materials usually have the characteristics of these types of phonon motion at the same time. The internal defects and discontinuous interfaces strengthen the phonon scattering, and the heat transfer efficiency can be significantly suppressed[91-93]. It should be noted that the thermal transport mechanism of organic materials is different from that of inorganic materials with crystalline structures. Therefore, phonon transport is almost carried out with no apparent scattering behavior, as shown in Figure 3D[78,93]. Figure 3E shows the phonon transport behavior in inorganic/organic hybrid materials. Generally, the phonon transport in hybrid materials is difficult to be directly predicted by the phonon transport mechanisms of conducting polymers and inorganic materials.
σ and S of pure or unprocessed conducting polymers are usually unsatisfactory. Rational doping can well tune n, which is closely related to σ and S. Doping methods and mechanisms of organic and inorganic materials are usually different, which are mainly derived from the different transport models and mechanisms between these materials. According to different doping mechanisms, there are many doping types, including chemical doping, optical doping, interface doping, and electrochemical doping. Chemical doping is based on the interaction between molecules, which can greatly change the properties of conducting polymers. Figure 4A indicates the main effect of chemical doping for conducting polymers, in which fillers with oxidation and reduction properties are introduced into polymers to increase the number of carriers, to increase σ. A typical example is a camphanic acid, a typical dopant to provide the electron for P3HT. Figure 4B shows a schematic diagram of mixed doping, in which the matrix material and the dopant are well mixed before deposition so that the dopant molecules are well dispersed in the matrix material. As can be seen, 2,3,5,6-Tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4TCNQ) as a dopant is uniformly dispersed in P3HT. As a result, such doping can greatly improve n. However, the materials prepared by this doping method cannot adapt to most solvents, and such a doping method is also difficult to restore the undoped morphology. It should be noted that this dopant might also affect the crystallinity of the polymer, which may result in the change of other properties. It was reported that with increasing the concentration of F4CNQ dopant, the aggregation of P3HT became more significant. Compared with their original state, the newly-formed complex P3HT chains are flatter. Also, the increased F4CNQ dopant could result in reduced crystalline domain size and increased amorphous pentacene phase, which caused the decrease of µ. Besides, F4CNQ anions mainly exist in amorphous regions of polymer films and side chains, which is possible to form π stacking eutectic phenomenon and, in turn, increase the µ. In terms of the sequential doping method based on the high-quality matrix material, the dopant can achieve good dispersion in the matrix material. Compared with previous doping, sequential doping can maintain the morphology of the matrix material and is also easier to follow-up processing. By using this doping method, the P3HT molecules can be wrapped by a group of doped ions, forming a discontinuous polymer structure. Such doping contributes to a much higher σ.
Figure 4. Schematic diagrams of (A) chemical doping in conducting polymers and (B) different specific embodiments and internal structure of doping. Reproduced with permission. Copyright 2020 Royal Society of Chemistry. TE: Thermoelectric; F4TCNQ: 2,3,5,6-Tetrafluoro-7,7,8,8-tetracyanoquinodimethane; P3HT: poly(3-hexylthiophene).
Conducting polymers are suitable for secondary doping to order their microstructures to improve the composition and morphology of conducting polymers without changing the doping level. Secondary doping can be followed by the doping operation to increase S and σ simultaneously. There are many types of pre- and post-treatments to achieve this goal. For example, polar solvent treatment can enhance the order of the polymer microstructure, such as dimethyl sulfoxide (DMSO) that is generally used to process PEDOT: PSS, and its σ can be improved by a hundred times. This is attributed to the high dielectric constant of DMSO and the induced strong screening effects. DMSO as a unary solvent treatment has been proven to increase σ without changing the doping level significantly, so the impact on S is negligible. Therefore, it is possible to improve performance by maintaining S value. In addition to polar solvent treatment, post-treatment is another effective way to order the microstructure of conducting polymers. During post-treatment, the excess insulating phase can be removed by phase segregation to increase σ. Commonly used post-treatment methods include employing DMSO, methanol, N,N-dimethylformamide (DMF) of CuCl2, formic acid, sulfuric acid[107,108], and then rinse. Taking PEDOT: PSS as an example, H3SO4+ and HSO4- can interact with positively charged PEDOT+ and negatively charged PSS-. By inducing phase segregation, part of the PSS is removed, which increases the possibility of PEDOT forming crystals. PSS and H2SO4 are removed by cleaning with excess deionized water. After rational post-treatment, the PEDOT has been reported with the highest σ of up to 4200 S cm-1. Pre-treatment is usually combined with post-treatment, which aims to improve S to improve S2σ, but it may cause potential intermediate damage on the microstructures of conducting polymers. Similar to post-treatment, pre-treatment can effectively improve the σ of the polymer. For example, pre-treatments such as nitrogen and argon use plasma to improve the surface properties of the fabric, including wettability, hydrophobicity, and dyeability. Besides, pre-treatments also include solvent treatment and oxidant treatment, which impact electrical and mechanical conductive polymers. Furthermore, sequential treatment combines secondary doping and doping, which simultaneously increases S and σ. As mentioned before, doping can tune the oxidation level to improve the band structure and density of states to improve S, while secondary doping cannot change the oxidation level of the polymer.
The energy filtering effect is proposed from the interfaces between different materials, and it can effectively improve S without reducing σ. Theoretically, the alternating energy barrier layer realizes a filter that only allows high-energy carriers to pass through, thereby increasing the entropy change of carrier transport. Generally, both inorganic materials such as superlattices[111,112] and organic-inorganic hybrid systems[113-115] can show significant energy filtering effects, especially for hybrid materials with obviously different band structures. For example, researchers used carbon nanotubes (CNTs) and redox graphene to dope conducting polymers such as PEDOT, PANI, and PPy. By the effective energy filtering, σ can increase by 1-2 orders of magnitude without decreases in S. However, it should be noted that the principle of energy filtering is still not very clear; therefore, it is usually difficult to find suitable hybrid materials to achieve high TE performance. Furthermore, in terms of the quantum confinement effect, when the sample size reaches the nanometer level, the electronic energy level near the Fermi level splits from a continuous state into a discrete energy level, and the physical property of the material significantly changes. However, the technology for preparing organic TE materials with orderly low-dimensional structure is not mature, limiting the possibility of its broad application. Therefore, the method to control the growth of materials at the molecular level is an important research direction for conducting polymer-based thermoelectrics.
With the development of conducting polymers-based TE materials, their TE performance has been greatly improved. To illustrate the progress clearly, we firstly make the following summary[46,50-52,54,55,121-175]: Table 1 provides the fundamental structures of conducting polymers; Table 2 summarizes the TE properties of different conducting polymers; Table 3 shows the performance of devices composed of conducting polymers.
Structure of conductive polymers for thermoelectric applications
|Name of the polymers||Structure of the polymers|
The thermoelectric properties of CPs developed in recent years
|Year||Sample||ZT||S2σ (μW m-1 K-2)||σ (S cm-1)||S (μV K-1)||κ (W m-1 K-1)||Ref.|
|2015||Bar-coated SWCNT/P3HT thin films||-||105||24.8 ± 9.9||60.7 ± 2.4||-|||
|2015||Spray-printed CNT/P3HT||-||325 ± 101||345 ± 88||97 ± 11||-|||
|2016||Highly anisotropic P3HT films||0.1||62.4||320||269||-|||
|2016||[Fe(TFSI)3]-doped P3HT powder||-||17.10||96.1||42.2||-|||
|2018||P3HT vapour-doped with F4TCNQ||-||3||22||60||-|||
|2018||F4TCNQ-doped P3HT Sb2Te3 based printed||-||1.6||1.6||102||-|||
|2019||P3HT/SWCNTs composite films by HClO4 post-treatment||-||27.99||0.6 ± 0.03||283 ± 17||-|||
|2020||Sequentially doped P3HT:F4TCNQ films||-||56||160||60||-|||
|2020||P3HT doping with a molybdenum dithiolene||-||160||260 ± 26||44||-|||
|2021||F4TCNQ-doped CNT yarn/P3HT||1.1||1640-2160||320||0.8||-|||
|2021||P3HT dual doping of Au metal precursors||-||110||207||73.9||-|||
|2021||Ternary design of P3HT||0.008||30||265||44||-|||
|2021||Ferric salt-doped P3HT||-||20||128||85||-|||
|2021||F6TCNNQ doped P3HT||-||80||500||45||-|||
|2015||Liquid exfoliated graphene doped PEDOT: PSS||0.05||53.3||160||50-100||-|||
|2016||CNT/PEDOT: PSS nanocomposite films||-||151 ± 34||780 ± 51||43.7 ± 3.3||-|||
|2016||Te-PEDOT: PSS composites||0.42||284||334.68||10.35||-|||
|2017||PEDOT: PSS/PANI-CSA multilayer||-||325||1680||44||-|||
|2018||Solvent-treated PEDOT: PSS thin films||-||245.58||1000||334.68||-|||
|2018||Post-treatment of CNT/PEDOT: PSS||-||83.2 ± 6.4||-||29.3 ± 2.1||-|||
|2019||PEDOT: PSS-coated Te nanorod||0.42||141.9||83.27||204.6||-|||
|2020||Wet‐spun PEDOT: PSS||0.1||30||830||19||-|||
|2020||PEDOT: PSS film by treatment with hydrazine||0.25||93.5||-||42.7||-|||
|2021||Acid-treatment of PEDOT: PSS/Carbon Dots||0.02||148.27 ± 20||1753.92||-||-|||
|2021||PEDOT: PSS/Cu2Se-based composite films||0.4||820||470||78.2||-|||
|2021||PEDOT: PSS/PVA/Te ternary composite fibers||-||8.5||382.4||18||-|||
|2021||PEDOT: PSS/SWCNT composites||-||182.7 ± 9.2||1602.6 ± 103||33.4 ± 0.4||-|||
|2021||PEDOT: PSS/Te nano-composite||0.355||154.2 ± 3||240||95.3 ± 3||0.12|||
|2021||PEDOT: PSS/Carbon Dots||-||148.27 ± 20||1753.92 ± 50||30||0.38|||
|2021||PEDOT: PSS films DMSO treatment||-||105.2||578||67||-|||
|2019||PANI/GO nanocomposite||0.4 (RT)|
|2021||PANI-coated Ag2Se nanowire||-||320||301.9||98||-|||
|2021||Carbon nanotubes/polyaniline||-||321 ± 24||3572 ± 78||33.3||-|||
Performance of flexible thermoelectric devices
|Year||Materials||Substrate||Couple number||ΔT (K)||Output voltage (mV)||Output power (μW)||Power density (μW cm-2)||Ref.|
|2014||Glass fabric + Sb2Te3||Glass fabric + Bi2Te3||Al2O3||8||50||80||-||3800|||
|2014||PI + Sb2Te3||PI + Bi2Te3||PI||7||50||80||1200||-|||
|2014||SWNT/PVDF/DMF composites||SWNT composites||Glass||-||50||0.9||0.6||-|||
|2015||PEDOT: PSS||Cu intercalated Bi2Se3/PVDF||Glass||-||15||1.3||-||1222|||
|2016||Bi/Te + CNTs||Bi/Te + CNTs||PDMS||-||333.15||920||0.57||4.5|||
|2016||Bi2Te3 + FPCB||Bi2Te3 + FPCB||FPCB||-||12||48||0.1306||0.67|||
|2017||NWPU/PEDOT: PSS/MWCNT||NWPU/N-doped MWCT||3D fabric||2||66||0.8||0.0026||-|||
|2019||PEDOT-Cl||Carbon fiber thread||Cotton fabrics||13||24||48.9||0.6935||-|||
|2019||CNTs and FeCl3||Polyethyleneimine/CNT||Glass||5||50||23||0.008||-|||
|2021||FeCl3-doped P3HT||Silver paste||-||-||23.3||-||0.00464||-|||
Polypyrrole (PPy) is a solid polymer formed by oxidative polymerization of pyrrole, which is widely used in electronics, optics, biology, and medicine[176,177]. The formulation of PPy is H(C4H2NH)nH. In 1919, Angeli and Pieroni reported the first batch of PPy examples of pyrrole black prepared by pyrrole magnesium bromide. Electrochemical synthesis and chemical oxidation are the most commonly used methods to fabricate PPy[179,180]. The chemical oxidation of pyrrole can be expressed as:
n C4H4NH + 2n FeCl3 → (C4H2NH)n + 2n FeCl2 + 2n HCl (3-1)
The mechanism of chemical oxidation is considered as the formation of pi-radical cation C4H4NH+. This electrophile attacks the C-2 carbon of the unoxidized pyrrole molecule, producing a dimeric cation [(C4H4NH)2]++. Thus, conductive forms of PPy are prepared by oxidation (“p-doping”) of the polymer, expressed as:
(C4H2NH)n + 0.2 X → [(C4H2NH)nX0.2] (3-2)
A high-performance PPy was discovered in 2017, fabricated by a chemical oxidation polymerization method. In this method, cetyltrimethyl ammonium bromide was dissolved in deionized water and then added to the pyrrole monomer. The black precipitates were obtained using deionized water and ethanol to wash the products generated from the oxidation reaction, as shown in Figure 5A. With increasing the polymerization time, the diameter of the PPy nanowires did not significantly change, but the curling degree of the nanowires was significantly decreased, as indicated in Figure 5B. Besides, the nanowires produced at 0.21 mol L-1 oxidant concentration were straighter than the products produced at 0.28 mol L-1 and
Figure 5. (A) Schematic illustration of the preparation process of PPy nanostructures by chemical oxidation polymerization; FESEM images of (B) products treated with oxidant concentration at 0.14 mol L-1 for 24 h; (C) Products treated with oxidant concentration at 0.21 mol L-1 for 8 h; (D) PPy prepared in pure EtOH; TE properties of σ, S, and S2σ of PPy nanowires prepared with (E) a polymerization time of 8 h under different APS concentrations, (F) different oxidants, and (G) in various reaction media. Reproduced with permission. Copyright 2017 Royal Society of Chemistry. PPy: Polypyrrole; APS: ammonium peroxydisulfate; TE: thermoelectric.
Moreover, the difference in the appearance of the product was caused by the difference in the reaction medium. The clear appearance of nanowires is formed by H2O:EtOH ratio (3:1). When pure EtOH was used, it formed a flat surface, as shown in Figure 5D. Figure 5E indicates the TE performance of PPy nanowires synthesized under different APS concentrations. When the concentration was 0.21 mol L-1, σ, S, and S2σ reach the maximum values, which are
In addition to these works, researchers are trying to break through the TE application limitations of PPy. For example, graphene was used to improve the TE performance of PPy nanowires. With increasing the content of graphene, S and σ were increased by 20%. Similarly, with increasing the temperature from 300 K to 380 K, S2σ showed the same trend. At 380 K, the material obtained the highest S2σ of 1.01 μW m-1 K-2, which was improved by 3.3 times compared with pure PPy nanowires. The performance of PPy nanotube, PPy nanowire, and PPy particle was also compared. Besides, by inserting PPy into reduced graphene oxide, graphene nanosheets were prevented from agglomerating while improving the carrier transport. As a result, good flexibility, good mechanical strength, and high σ were achieved. The prepared samples had an S2σ 135 times higher than that of the pure PPy nanotube at room temperature, and exhibited high TE stability after repeated bending.
Like adding graphene, single-walled carbon nanotubes (SWCNT) were used to improve the TE properties of PPy. An in-situ polymerization method was used to induce PPy to grow along the regular SWCNT surface. No significant changes in κ were observed, but the ZT was 55 times higher than that of pure PPy. Moreover, PPy and silver were composited into a thin film through a simple nature-friendly optical-chemical process. By changing the concentration and size of Ag particles in the PPy substrate, σ was increased from 1.5 S cm-1 to 17.3 S cm-1, and κ was decreased to 0.16 W m-1 K-1. S was slightly decreased in the process. As a result, the ZT of this material reached the maximum value of ~7.4 × 10-3 at 355 K. After integrating six groups of thin films into devices, the maximum voltage can reach 6 mV at room temperature, and the output power is 30 ×10-6 μW. In addition to Ag, Te was also added to the pyrrole polymerization process to improve the crystal structure, morphology, optical, and electrical properties, leading to an S2σ of 23.89 μW m-1 K-2, 850 times higher than pure PPy.
Apart from hybrid/composite methods, doping is also used to improve the performance of PPy. For example, FeCl3 can be used as an oxidant, and p-toluene sulphonic acid (PTSA) can be used as a dopant. When the ratio of PTSA was increased, σ was increased from 4.8 S cm-1 to 162.7 S cm-1. The highest S2σ can reach 0.45 μW m-1 K-2. Subsequently, seven sets of films were used to prepare the corresponding wristband-type devices. The maximum open-circuit voltage and current reached 336 mV at a ΔT of 80 K, revealing the possibility of PPy as a core material in wearable devices.
PANI is a rod-shaped flexible organic material and has attracted significant attention since the 1980s. Chemical or electrochemical methods are widely used to synthesize PANI. PANI is difficult to degrade, and it can be doped and de-doped easily by treatment with aqueous acid and base. The chemical reaction in PANI can be expressed as:
n C6H5NH2 + [O] → [C6H4NH]n + H2O (3-3)
where [O] is a universal oxidant. The synthesis of PANI is facile, but the reaction mechanism is complicated. Regarding the TE applications of PANI, recent works mainly focus on the hybrid materials composed of CNTs and PANI and the hybridization of inorganic materials and PANI. For example, an outstanding PANI-based material composed of SWCNT and PANI was reported in 2018. The maximum S2σ can reach 100 μW m-1 K-2 with an ultra-high σ of 4000 S cm-1 at 410 K, which is the highest value until now. Figure 6A illustrates the fabrication of PANI/SWCNT hybrids. A typical solution-based synthesis route with a drop-casting method was developed to prepare the flexible thin films. With the increase of CNTs, the film thickness was increased. Figure 6B is the SEM image of the cross-section view of the thin film with 90 wt% SWCNT. When the content of SWCNTs was < 10 wt%, some independent SWCNTs or nanotube clusters were isolated by the polymer coating, which affected the connection between SWCNTs and in turn σ. However, when the content was at 10-90 wt%, σ was significantly increased since σ was dominated by the three-dimensional interconnect structure of SWCNTs, as illustrated by Figure 6C. After 100 manual bends, S and σ values were kept stable [Figure 6D]. When the reaction time is 12 h, S2σ reaches the maximum value of ~2 μW m-1 K-2, as shown in Figure 6E. Figure 6F-G shows the TE performance as a function of the CNT content. All TE properties show the best values at ~60 wt% SWCNTs, indicating that a rational design of SWCNT content is crucial for improving the TE performance of PANI. The output voltage can reach 0.047 μW at a ΔT of 75 K in the as-fabricated F-TEG.
Figure 6. (A) Schematic diagram of the preparation of PANI film; (B) SEM cross-sectional image of the composite film with 90 % SWCNT; (C) schematic diagram of electron transport of the composite film when the content of SWCNT is > 10 %; (D) illustrations of the bending experiment, the maximum bending radius are r = 2 mm; (E) S2σ for different polymerization time; (F) σ and S and (G) S2σ as a function of the content of CNTs. Reproduced with permission. Copyright 2018 Royal Society of Chemistry. PANI: Polyaniline; SWCNT: single-walled carbon nanotubes; CNTs: carbon nanotubes.
Apart from the above case, there is SWCNT and sulfite-sulfonic acid-treated PANI. The strong interfacial interaction allowed PANI to grow regularly on the surface of SWCNT, leading to a ZT of 0.01 at room temperature. Ethanol was used to treat PANI/SWCNT composites. The ethanol treatment allowed PANI to be partially de-doped, leading to significantly improved S. Although this treatment reduced σ to some extent, there was also a high S2σ of 365 μW m-1 K-2. In the developed device, the output power of 2.86 μW was obtained at a ΔT of 50 K. In addition to the cases of PANI/SWCNT, flexible three-dimensional graphene/PANI hybrid material was fabricated by a chemical vapor deposition method using a particulate nickel catalyst as support, which showed excellent σ, S, and high flexibility during bending. After repeated bending tests, the maximum S2σ reached 81.9 μW m-1 K-2, which maintained more than 80 % performance.
PEDOT is a polymer-based 3,4-ethylenedioxythiophene (EDOT), which was first reported by Bayer AG in 1989. Compared with other polythiophenes, PEDOT has optical transparency, high stability, medium energy gap, low redox potential, and poor water solubility[194,195]. Therefore, PEDOT is usually used as a composite material to form PEDOT: PSS. This polymer is produced by oxidation, and the process starts with the formation of free radical cations [C2H4O2C4H2S]+ of the EDOT monomer. Thus, the ideal conversion with peroxodisulfate can be expressed as:
n C2H4O2C4H2S + n (OSO3)22- → [C2H4O2C4S]n + 2n HOSO3- (3-4)
Regarding the application of PEDOT in thermoelectrics, PEDOT shows many advantages, including good forming ability by versatile fabrication techniques, superior optical transparency in visible light range, high electrical conductivity and intrinsically high work function, and good physical and chemical stability in the air. PEDOT was reported to be used in coated textiles, prepared by a vapor phase polymerization technique. Three different types of fabrics, including cotton thread (CO), cotton textile (CT), and model textile (MT), were used to evaluate the performance. As shown in SEM images in Figure 7A-C, the regularity and surface characteristics of MT are better than the CO and CT. In the un-extended state, PEDOT polymerizes uniformly and neatly on the textile surface. When the stretch rate reaches 30%, there are only some micro-cracks, and when the stretch rate reaches 50%, PEDOT partially peels off, and the electron transport may be slightly affected. Figure 7D indicates the variation of S for three different types of fabric in different deposition cycles. The value of S fluctuates between 13-16 μV K-1, but the value is influenced by the number of deposition. The stability of S and resistance (R) of the as-fabricated materials based on different heat treatment temperatures are shown in Figure 7E, in which the stability of R and S based on the MT-type PEDOT fabric is acceptable at low heat treatment temperatures. Figure 7F shows temperature-dependent S of pristine and stretched materials, from which S increases with increasing the temperature for both pristine and stretched MT fabric. Figure 7G shows the schematic diagram of the as-fabricated F-TEG and the photos showing its size and surface, from which high flexibility can be observed. Figure 7H shows its output voltage and power. An output voltage of > 20 mV, as well as an output power of ~0.07 μW, can be achieved at a ΔT of 100 K. By wearing the device on the knee, the resistance changes when the knee is bent and upright, from which the device exhibits considerable repeatability in a certain period [Figure 7I].
Figure 7. SEM images of (A) cotton thread (CO)-based; (B) cotton textile (CT)-based; and (C) model textile (MT)-based PEDOT; (D) the S of the hybrids as a function of the number of deposition cycle; (E) resistance change (ΔR/R0) and S change (ΔS/S0) with different heat treatment temperatures; (F) temperature-dependent S of pristine and stretched material; (G) schematic diagram of the as-fabricated F-TEG and the photos showing its size and surface; (H) the performance of the F-TEG, and (I) the resistance and time when the device is bent and straight. Reproduced with permission. Copyright 2019 Royal Society of Chemistry.
Recently, an ultra-fine PEDOT was fabricated using a homemade micellar soft-template method with a high σ value of 1340 S cm-1 obtained. After treatment with NaOH and H2SO4, S2σ reached 46.51 μW m-1 K-2 at room temperature. Compared with the traditional preparation methods, the performance was improved by 54%. After connecting six strips in series, the output power can reach 0.157 μW at a ΔT of 51.6 K, indicating that the film made by PEDOT nanowire has the potential to be employed in wearable devices. Moreover, controlled template-free in-situ polymerization of PEDOT was also studied to enhance the TE performance of the textile sublayer. A simple one-bath template-free solution method was reported to fabricate PEDOT with an σ value of up to 560 S cm-1 and an S2σ value of 0.9 μW m-1 K-2 at room temperature. Currently, the giant photo-magneto-TE effect was used to optimize the PEDOT grown orientation. It is worth noting that tosylate was synthesized using monomer seeds that were complexed through pyridine units to 3D tectons on graphene via surface-confined host-guest chemistry. At 300 K environment, EPG which was PEDOT:Tos coated by ZnPc:EDOT-Py/lean-mix concrete type of material (TSB)/unmodified graphene showed a great TE performance with S2σ = 0.00115 μW m-1 K-2 and ZT = 0.35.
PEDOT: PSS is a polymer composed of two ionomers. One is sulfonated polystyrene, and the other one is PEDOT. PEDOT: PSS can be obtained by mixing an aqueous solution of PSS with EDOT monomers and then adding Na2S2O8 and Fe2(SO4)3 solution[201,202]. In terms of applying PEDOT: PSS as TE materials, rational pre- and post-treatments were commonly used to boost the TE performance of PEDOT: PSS. A triple post-treatment was developed to achieve an extraordinary TE performance in PEDOT: PSS thin films, as illustrated in Figure 8. Figure 8A shows the XRD results for PEDOT: PSS films with different treating conditions, including treating with CH3NO, CH3NO + H2SO4, and CH3NO + H2SO4 + NaBH4, respectively. As can be seen, the peak values of PEDOT: PSS vary for different processing methods. Compared with the original sample, the intensity of (100) diffraction peak is significantly increased after treating with H2SO4, indicating significantly improved order in the as-fabricated thin films, as illustrated by the embedded figure in Figure 8A. Figure 8B shows the XPS results of the thin films with different treatments. After the treatment with CH3NO and H2SO4, the mass ratio between PSS and PEDOT decreased, indicating that the rational post-treatment can achieve the selective removal of the PSS content in the film. Therefore, it can be concluded that the decrease in binding energy changes the average oxidation level. Figure 8C is the SEM image of the as-fabricated thin films after different treatments. After removing excess PSS, the cross-section shows an increasingly ordered microstructure. After the triple post-processing, the σ can be significantly improved up to 1786 S cm-1, and S can reach 28.1 μV K-1 at room temperature. The corresponding F-TEG using polyimide as substrate and copper wire as electrodes and n-type legs showed the maximum power density measured was 1 μW cm-2 when the device was attached to the human arm.
Figure 8. (A) XRD results for PEDOT: PSS films with different treating conditions within schematic diagram of PEDOT: PSS; (B) XPS results of PEDOT: PSS film with different treating conditions; (C) SEM images of cross-sectional PEDOT: PSS thin films after different treatments. Reproduced with permission. Copyright 2019 ACS Publications. (D) Measured σ, S, and S2σ of tetrakis(dimethylamino)ethylene (TDAE)-treated PEDOT: PSS after different treatment durations; (E) Schematic diagram of the flexible TE module fabricated by PEDOT: PSS; (F) output power density and voltage as a function of the current. Reproduced with permission. Copyright 2020 Royal Society of Chemistry. (G) TEM image of PEDOT: PSS films with 6 wt% Cu-Bi0.5Sb1.5Te3 filler incorporation; (H) images of the as-fabricated F-TE, and its thermovolta2021/9/29ge generations with human wrist and chest as thermal sources; (I) measured thermovoltage using a heating plate, human wrist, and chest as thermal sources. Reproduced with permission. Copyright 2020 ELSEVIER. PEDOT: PSS: Poly(3,4-ethylenedioxythiophene)poly(styrenesulfonate).
In addition to employ CH3NO, H2SO4, and NaBH4 as treatment, ethylene glycol (EG) pretreatment, H2SO4 post-treatment, and tetrakis(dimethylamino)ethylene (TDAE) post-treatment were also employed in PEDOT: PSS in sequence. σ can reach about 1333 S cm-1 after EG pre-treatment, mainly due to the damping caused by the excessive non-ionized PSS in the film. The post-processing of H2SO4 can further boost σ up to 4000 S cm-1 since H2SO4 can order the microstructure of PEDOT: PSS. After coupling with TDAE treatment, a maximum S2σ of 37.2 μW m-1 K-2 can be achieved [Figure 8D]. The as-fabricated device was designed according to the principle of the solar absorber and used the heat provided by solar energy to form a temperature gradient at both sides of the device, thereby leading to a high output power density. Figure 8E is a conceptual diagram of this device. In the actual test, the hot side was heated by solar energy to 356 K while the cold side maintained a temperature of about 300 K. Therefore, based on the thermodynamic numerical analysis, the power density of a 20 μm thick film can reach 5.12 μW cm-2 at a ΔT of 56 K. Figure 8F is the relationship diagram of output voltage, power density and current, which fully embodies the application potential of the optimized films.
In addition to pure PEDOT: PSS thin films, the hybrids of organic and inorganic materials have improved TE performance. For example, a thin-film material with high crystallinity was obtained by combining
In addition to studies of PEDOT: PSS films, one-dimensional PEDOT: PSS fibers are also widely reported. By using a continuous wet spinning process and treating with sulfuric acid, the TE performance of the PEDOT: PSS fibers can be optimized. Figure 9A shows a schematic diagram of the separation of PSS in the fiber during H2SO4 treatment. Figure 9B is a partially enlarged SEM image after H2SO4 treatment. As can be seen, the microscopic morphology of the fiber shows inapparent change before and after the H2SO4 treatment. However, the diameter decreases obviously because the PSS in the fiber is partially removed. The observed S2σ value is directly related to the processing time of H2SO4 [Figure 9C]. When H2SO4 was processed for 10 min, S2σ reached its maximum value. Besides, a standard tensile test was employed to evaluate the mechanical properties of PEDOT: PSS fibers and the results are shown in Figure 9D. As can be seen, the mechanical properties of the post-treated PEDOT: PSS fibers are better than those of the untreated fibers, and the mechanical properties of the untreated fibers are better than that of the treated film material. Figure 9E shows the measured performance of a device composed of 5 pairs of p(PEDOT: PSS)-n(Ni) junctions. The maximum output power can reach 0.0051 μW at a ΔT of 10 K. Figure 9F is the stitching of the device to the earphone. When ΔT is ~9.1 K, the maximum power density can reach 0.273 μW cm-2, which is comparable to the performance of Bi2Te3-based materials. A novel F-TEG can be designed on cotton fibers using PEDOT: PSS as p-type materials and CNTs as n-type materials. Figure 9G is the comparison of σ and S of materials with different cotton fiber content. The largest σ can reach 871 S cm-1, and S can reach 58 μV K-1. Figure 9H is the schematic diagram and photos of the device. Figure 9I illustrates the output power can reach 380 μW at a ΔT of 60 K. Combing CNT and PEDOT: PSS using wet-spinning and post-processing, the resulted p- and n-type S2σ can reach 83.2 ± 6.4 and 113 ± 25 μW m-1 K-2, respectively. When 12 pairs of p- and n-type fibers were used to make a device, the maximum output power can be observed at 430 μW at a ΔT of 10 K, suggesting that the PEDOT: PSS fibers to be employed in wearable electronics.
Figure 9. (A) Schematic diagram of PEDOT: PSS fiber treated by H2SO4; (B) Partially enlarged SEM image of PEDOT: PSS fiber; (C) Effect of H2SO4 treating time on the S2σ fiber; (D) Evaluation of mechanical properties of PEDOT: PSS fiber and film by post-treatment; (E) Performance of fiber-based F-TEG under a ΔT of 10 K; (F) Practical application of the fiber-based device. Reproduced with permission. Copyright 2020 ELSEVIER. (G) S and σ of fiber-based materials with different contents of cotton fiber; (H) schematic diagram and photos of the as-fabricated device, and (I) Relationship between device performance and ΔT. Reproduced with permission. Copyright 2020 ELSEVIER. PEDOT: PSS: Poly(3,4-ethylenedioxythiophene)poly(styrenesulfonate); F-TEG: flexible TE generator.
P3HT is a 3-hexylthiophene polymer derived from polythiophenes. P3HT is a colored solid and easily soluble in organic solvents. P3HT was first synthesized in the 1980s. There are various synthetic methods to fabricate P3HT, including electropolymerization, oxidation (mainly by FeCl3), nickel catalysis (McCullough, Rieke, GRIM), Pd catalysis (Suzuki and Stille coupling), and recent direct arylation Aggregation (DArP).
Research on the thermoelectricity of P3HT was almost relevant to F4TCNQ doping. For example, it was reported that by doping F4CNQ into P3HT through a vapor phase infiltration, its TE performance was improved. Figure 10A shows the schematic diagram of the vapor phase doping method and the chemical structures of P3HT and F4TCNQ. Based on morphology, doping can make the material exhibit better conductivity under the same doping concentration. Similarly, in the solution doping, P3HT and F4CNQ are aggregated due to charge transfer, which directly affects the different morphologies in the film. Therefore, some products have poor structural domains at the same doping level, resulting in differences in σ. Regarding the specific content, the σ value by vapor phase doping was 48 times higher than that of the solution doping. In terms of the achieved S and σ, they can reach 85 μV K-1 and 10 S cm-1 in vapor-doped P3HT. In contrast, by solution doping, the S is 100 μV K-1, but the σ is only 10-5-10-3 S cm-1. As shown in Figure 10B, the S2σ by vapor phase doping is much better than solution doping. In addition to this case, plenty of studies have been using F4CNQ as a dopant for P3HT. For example, the influences of controlling chain alignment and crystallization on S2σ of P3HT were reported with F4CNQ as the dopant. Higher in-plane orientation and higher doping concentration can lead to the semi-crystalline structure of aligned P3HT, which contributes to better TE performance than the smectic-like phase. The highest σ can reach
Figure 10. (A) Schematic diagram of the vapor phase doping method and the chemical structures of P3HT and F4CNQ; (B) comparison of TE performance between vapor phase doping and solution doping for P3HT. Reproduced with permission. Copyright 2018 ACS Publications. (C) Schematic diagram of the synthesis of the P3HT/CNT composite film composed of CNTs with different diameters and different contents; (D) SEM image of the hybrid film with 95 wt% P3HT; (E) S2σ of the hybrid film as a function of P3HT content. Reproduced with permission.Copyright 2018 The Royal Society of Chemistry. P3HT: Poly(3-hexylthiophene); CNTs: carbon nanotubes.
In addition to the research on F4CNQ-doped P3HT, CNT/P3HT composite materials are also in popularity, from which the good performance is benefitted from the unique structure and excellent electron transport performance of CNT itself. For example, composite films with different diameters were prepared [Figure 10C]. As a result, 40 wt% of CNTs were reported to be uniformly dispersed in the composite material, but the optimal TE performance was not achieved. Regarding the selection of the diameter of CNTs, the diameter of CNTs of < 15 nm was the best, and the maximum σ can reach
In addition to PPy, PANI, PEDOT, PEDOT: PSS, and P3HT, other conducting polymers such as polyvinylidene fluoride (PVDF), Poly[Kx(nickel-ethylenetetrathiolate)], and polystyrene (PS) are also reported to have potential research possibilities. For example, PVDF can compound with Ag2Se nanowires to form a free-standing composite film. Figure 11A shows a typical preparation processing. Figure 11B is an SEM image of the fabricated composite film, in which a grape-like structure can be seen. Its TE performance is shown in Figure 11C. At 300 K, S2σ can reach 189.02 μW m-1 K-2, and ZT reached 0.008. After 1000 bending cycles, the conductivity only drops by 15.8% [Figure 11D] due to the entanglement of the two materials in the structure. Figure 11E is the as-fabricated F-TEG assembled with five sets of products where the joints are made of copper foil and silver. Figure 11F shows the device’s performance. When the temperature was increased, the resistance significantly dropped, and the output power continued to rise, reaching the maximum value at 30 K. An output power of 0.005 μW can be obtained. In addition to compounding with Ag2Se, a study about Bi2Se3/PVDF composite was reported. κ of this composite was significantly lower than that of Bi2Se3, which was only 0.06 W m-1 K-1 at 300 K, and the ZT value was ~0.004.
Figure 11. (A) Schematic diagram of the synthesis of PVDF/Ag2Se composite film; (B) partially enlarged SEM image of thin-film with 1:9.5 mass ratio of PVDF/Ag2Se; (C) schematic diagram of the relationship between ZT and material mass ratio, the insets show the photos of the as-fabricated flexible films; (D) specific bending test of the film; (E) the as-fabricated device composed of 5 groups of PVDF/Ag2Se composite films; (F) corresponding device performance. Reproduced with permission. Copyright 2020 ACS Publications. PVDF: Polyvinylidene fluoride.
Figure 12. Strategies and outlooks for conducting polymer-based TE materials and devices. Optimization strategy. Reproduced with permission. Copyright 2021 Nature Portfolio. Test equipment. Reproduced with permission. Copyright 2020 ELSEVIER. Commercial TE devices. Reproduced with permission. Copyright 2021 ACS Publications. p-type and n-type principles. Mechanism of Peltier effect and device geometry. Reproduced under the terms of the Creative Commons Attribution License (CC BY). Copyright 2021 frontiers. Cooler. Reproduced with permission. Copyright 2018 Nature Portfolio. TE: Thermoelectric.
In addition to the research on PVDF-based TE materials, the TE potential of PS was also studied. PS was used to realize the condensation of the CNT conductive network as a binder to maintain the microstructure of the material. Compared with pure CNT, the film made of PS exhibited higher σ and S2σ. When the CNT concentration reaches 75%, S2σ can reach 789 μW m-1 K-2. Similar research reported that a device made of PS-based TE materials could show an output power density of 5.5 μW cm-2 under a ΔT of 70 K. Another popular TE polymer with great research value is the Poly[Kx(nickel-ethylenetetrathiolate)]. This type of n-type material based on nickel and polyurethane has been widely studied in recent years. For example, an n-type composite film can withstand 50% of the deformation, and its S was about 40 μV K-1 with a σ of
Organic TE materials show good flexibility and promising TE performance. Therefore, many different types of conducting polymer-based TE materials, including PPy, PANI, P3HT, PEDOT, and their hybrid/composite materials based on metal-organic complexes, are investigated. Among them, PANI and PEDOT: PSS show very high σ exceeding 4000 S cm-1, and their developed devices also show high power output. So far, the reported highest TE performance of conducting polymers was formed by the hybridization of PEDOT and Bi2Te3. This hybrid has an ultra-high S2σ with a value of 1350 μW m-1 K-2, and the ZT gets up to 0.58 at room temperature. As for the power density, one outstanding PEDOT: PSS was reported to have a value of 1200 μW cm-2 at a ΔT of 50 K.
According to the previous studies, a few challenges still exist in materials, devices, and test methods. In terms of material, the existing p-type conducting polymer-based TE materials still show limited TE properties compared to their inorganic counterparts, and the current strategies such as doping, hybridization/compositing, and post-treatment still show limited effects. Furthermore, the charge transport mechanisms are not clear, and the modeling is limited by the current technique. One significant shortage is that it is difficult to link the micro/nanostructure to their TE properties, especially for κ. Besides, the development of n-type conducting polymer-based TE materials is still challenging, and their TE performance is not stable enough. Other problems in materials are practical performance, such as their costs, stability, and flexibility, which are all challenges in the current applications. Regarding the devices, in addition to their poor performance, there is a lack of mature design rules for F-TEGs, such as the topological design, suitable substrates, and electrodes, as well as their durability and comfortability when wearing by human skin. In terms of efficiency, all these parameters, including interface resistance, interface thermal resistance, material aggregation structure, bending, and folding, affect the performance of the device, but the evasion and optimization of these influencing factors still cannot find effective rules. Furthermore, in terms of the test methods, κ of the conducting polymer-based TE materials is historically tricky due to the limitation of the evaluation technique. There is also a lack of computational-assisted methods to design conducting polymer-based devices since the current computation-based calculations such as first-principles and finite element analysis are mostly based on inorganic materials.
For n-type materials, the optimization can generally start from molecule design, doping, and treatment methods. Molecule design is possible to induce the difference between molecule stacking and morphology. Rigid skeleton structure is a popular direction of current research, which is considered to optimize carrier transport[224-226]. Besides, the optimization of the skeleton can adjust the lowest energy unoccupied molecular orbital energy level of the doping system, which improves the doping efficiency and stability. It is also essential to develop more suitable dopants because the miscibility between the dopant and the host conducting polymers affects the structural arrangement of the matrix directly, as well as the degree of energy level matching[227,228]. The current processing method mainly relies on encapsulation, which is possible to improve the stability of the n-type conducting polymer materials. However, to realize further optimization of n-type conducting polymers, structure improvement and reasonable design are still significant. For p-type conducting polymers, the research at this stage is relatively mature. However, there are still possibilities to improve the TE performance of p-type conducting polymers, which benefitted from the development of the TE mechanism for conducting polymers. Similar to n-type, current research of p-type conducting polymers can still optimize from morphology, doping level, crystallinity, and side chain.
Generally, ZTs of conducting polymers determine the maximum performance of devices. However, the device structure also directly impacts the energy conversion efficiency. Therefore, future research can focus on device assembly, including serial, folding, and stacking routes. Usually, the performance is serial > folding > stacking routes. Therefore, to maximize the device performance, selecting serial and increasing p-n couple is inevitable. Moreover, the volume of the devices increases and affects the actual application seriously. Therefore, to optimize the device performance, transplanting the construction methods such as Y-type or π-type can be extended the design of conducting polymers-based TE devices with high energy conversion efficiency.
Because ZT is determined by S, σ, and κ, it is crucial to develop a testing method to measure these parameters accurately. The four-point probe is mature for testing σ, while S evaluation relies on temperature difference and the voltage difference between the two sides of the sample. Since most of the samples of conducting polymers are thin films, the process, morphology, and size seriously affect the accuracy of ΔT measurement. Otherwise, the high impedance brought by low conductivity is also a difficult problem for testing S. Therefore, exploiting new methods and instruments to precise S is indispensable. For example, based on the Thomson effect, using an ac-dc technique to precise S is an ideal method. With regards to κ, there are standard steady-state absolute measurement, Ångström method, hot-strip (THS) method, etc. However, current measurements are still difficult to limit the error to 5%. Therefore, exploiting new methods to match different conducting polymers is the trend of development. As well, it is difficult to link the micro/nanostructures to the properties for conducting polymers. The studies of micro/nanostructures reveal the essence of boosting the performance of conducting polymers, such as the crystallinity that significantly affects the σ and the micro/nanoscale imperfects or defects that greatly influence the κ. Developing advanced micro/nanoscale characterization techniques such as high-resolution electron scanning/transmission microscopies are potential ways to solve this issue.
Wearable F-TEGs with high power generation can be used to charge wearable/portable electronics with low energy demand and the vehicle industry. It should be noted that although the performance is still unsatisfactory for current F-TEGs that rely on conducting polymers, PEDOT: PSS has already exhibited great potential to meet the power supply for low-power electronical equipment. Furthermore, if F-TEGs with non-toxic and wear-resistant features can be made into wristbands or clothing to supply power for electronic watches or other portable electronic devices by absorbing human body heat, it will be a leap forward for the entire industry.
Since the inadequate performance of current-conducting polymers, it is still difficult to apply conducting polymers on TE coolers. However, there is the cooler research about Poly(Ni-ett) with relatively high ZT (~0.3). With the analysis of infrared imaging technique, the maximum ΔT can be up to 41 K at the two contacts and cooling of 0.2 K even under heat-insulated conditions. According to the cooling coefficient of performance, ZT directly influences the efficiency of TE coolers. Therefore, this value is still the essential prerequisite for conducting polymers used in TE coolers, which is the critical content of future research.
Made the literature review and drafted the original version: Cao T, Shi XL
Revised the manuscript: Chen ZG, Zou J
Conceived and supervised the project: Chen ZGAvailability of data and materials
Not applicable.Financial support and sponsorship
This project was financially supported by the Australian Research Council and Innovation Centre for Sustainable Steel Project.Conflicts of interest
All authors declared that there are no conflicts of interest.Ethical approval and consent to participate
Not applicable.Consent for publication
© The Author(s) 2021.
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