Abstract:Flexible
thermoelectric materials and devices show great potential
to solve the energy crisis but still face great challenges of high
cost, complex fabrication, and tedious postprocessing. Searching for
abnormal thermoelectric materials with rapid and scale-up production
can significantly accelerate their applications. Here, we develop
superlarge 25 × 20 cm2 commercial graphite-produced
composite films in batches, achieved by a standard 10 min industrial
process. The high cost effectiveness (S
2σ/cost) of 7250… Show more
“…With increasing the Δ T up to 74 K, a V oc was increased to 14 mV. Figure 6f shows the V oc as a function of load resistance at a Δ T of 25 K. [ 9 ] When the load resistance was close to the internal resistance of the device, the maximum output power was 2.8 nW at a Δ T of 25 K. After calculation, the corresponding power density is 2.56 µW cm –2 . Our work indicates great application potential for sustainably charging low‐grade wearable electronics.…”
Section: Resultsmentioning
confidence: 99%
“…[ 5–8 ] Their thermoelectric potential can be evaluated by the dimensionless figure‐of‐merit ZT = S 2 σT / κ , where S , σ , T , and κ are the Seebeck coefficient, electrical conductivity, absolute temperature, and thermal conductivity, respectively. [ 9,10 ] The S 2 σ is described as the power factor for thermoelectric materials. Generally, traditional thermoelectric materials are mostly solid‐state inorganics, [ 11 ] such as GeTe, [ 12–14 ] Cu 2 Se, [ 15 ] and SnSe [ 16 ] that which reported excellent thermoelectric properties with ZT s > 2.…”
Owing to intrinsically high electrical conductivity and low thermoelectric conductivity, poly(3,4‐ethylenedioxithiophene):poly(styrenesulfonate) (PEDOT:PSS) shows promising thermoelectric properties. However, its relatively low power factor limits the practical applications of PEDOT:PSS. Here, unique dual post‐treatments by sodium sulfite (Na2SO3) and formamide (CH3NO) to boost the thermoelectric performance of flexible PEDOT:PSS films with an optimized power factor of 74.09 µW m–1 K–2 are used. Comprehensive characterizations confirm that CH3NO reduces the excessive insulating PSS and thereby increases the electrical conductivity, while Na2SO3 lowers the reduction of the doping level of PEDOT, leading to an increased Seebeck coefficient. Furthermore, the rationally post‐treated PEDOT:PSS films are assembled into a flexible thermoelectric device that exhibits an open‐circuit voltage of 2.8 mV using the heat from the human arm and an output power density of 2.56 µW cm–2 by a temperature difference of 25 K, indicating great potential for practical applications on sustainably charging low‐grade wearable electronics.
“…With increasing the Δ T up to 74 K, a V oc was increased to 14 mV. Figure 6f shows the V oc as a function of load resistance at a Δ T of 25 K. [ 9 ] When the load resistance was close to the internal resistance of the device, the maximum output power was 2.8 nW at a Δ T of 25 K. After calculation, the corresponding power density is 2.56 µW cm –2 . Our work indicates great application potential for sustainably charging low‐grade wearable electronics.…”
Section: Resultsmentioning
confidence: 99%
“…[ 5–8 ] Their thermoelectric potential can be evaluated by the dimensionless figure‐of‐merit ZT = S 2 σT / κ , where S , σ , T , and κ are the Seebeck coefficient, electrical conductivity, absolute temperature, and thermal conductivity, respectively. [ 9,10 ] The S 2 σ is described as the power factor for thermoelectric materials. Generally, traditional thermoelectric materials are mostly solid‐state inorganics, [ 11 ] such as GeTe, [ 12–14 ] Cu 2 Se, [ 15 ] and SnSe [ 16 ] that which reported excellent thermoelectric properties with ZT s > 2.…”
Owing to intrinsically high electrical conductivity and low thermoelectric conductivity, poly(3,4‐ethylenedioxithiophene):poly(styrenesulfonate) (PEDOT:PSS) shows promising thermoelectric properties. However, its relatively low power factor limits the practical applications of PEDOT:PSS. Here, unique dual post‐treatments by sodium sulfite (Na2SO3) and formamide (CH3NO) to boost the thermoelectric performance of flexible PEDOT:PSS films with an optimized power factor of 74.09 µW m–1 K–2 are used. Comprehensive characterizations confirm that CH3NO reduces the excessive insulating PSS and thereby increases the electrical conductivity, while Na2SO3 lowers the reduction of the doping level of PEDOT, leading to an increased Seebeck coefficient. Furthermore, the rationally post‐treated PEDOT:PSS films are assembled into a flexible thermoelectric device that exhibits an open‐circuit voltage of 2.8 mV using the heat from the human arm and an output power density of 2.56 µW cm–2 by a temperature difference of 25 K, indicating great potential for practical applications on sustainably charging low‐grade wearable electronics.
“…Further details can be consulted from our previous work. 27 4.3. Fabrication of the Thermoelectric Device.…”
Section: Discussionmentioning
confidence: 99%
“…Historically, some newly developed carbon materials such as graphene and carbon nanotubes (CNTs) have been studied to explore their thermoelectric potential. − However, these materials are relatively expensive; therefore, conventional carbon materials that can realize an industrial scale are valuable for practical thermoelectric applications and future commercialization. In this regard, developing efficient fabrication techniques, rising cost-effectiveness, and improving the thermoelectric performance become the three main goals for conventional carbon-based thermoelectrics that target industrial feasibility. − …”
Section: Introductionmentioning
confidence: 99%
“…Historically, conventional carbon-based materials developed for thermoelectric applications include natural graphite, expanded graphite, and carbon black . Among the conventional carbon-based materials, expanded graphite (EG) with a three-dimensional (3D) worm-like morphology is commercially massively available because of its cheap price. − Nowadays, the preparation of EG is relatively mature.…”
Due
to their cost-effectiveness and industry-scale feasibility,
carbon-based composites have been considered to be promising thermoelectric
materials for low-grade power generation. However, current fabrications
for carbon-based composites are time-consuming, and their thermoelectric
properties are still low. Herein, we develop an ultrafast and cost-effective
hot-pressing method to fabricate a novel carbon-based hybrid film,
which consists of ionic liquid/phenolic resin/carbon fiber/expanded
graphite. This method only costs no more than 15 min. We found that
the expanded graphite as the major component enables high flexibility
and the introduction of phenolic resin and carbon fiber enhances the
shear resistance and toughness of the film, while the ion-induced
carrier migration contributes to a high power factor of 38.7 μW
m–1 K–2 at 500 K in the carbon-based
hybrid film. After the comparison based on the ratios between the
power factor with fabrication time and cost among the current conventional
carbon-based thermoelectric composites, our hybrid films show the
best cost-effective property. Besides, a flexible thermoelectric device,
assembled by the as-designed hybrid films, shows a maximum output
power density of 79.3 nW cm–2 at a temperature difference
of 20 K. This work paves a new way to fabricate cost-effective and
high-performance carbon-based thermoelectric hybrids with promising
application potential.
Solid‐state bismuth telluride‐based thermoelectric devices enable the generation of electricity from temperature differences and have been commercially applied in various fields. However, in many scenarios, the surface of the heat source is not flat. Therefore, it is crucial to develop flexible thermoelectric materials and devices to efficiently utilize heat sources and expand their applications. Compared with organic thermoelectric materials and devices, inorganic flexible thermoelectric materials and devices have much higher thermoelectric performance and stability. Considering the rapid development in this research field, we carefully summarize the design principles, structures, and thermoelectric properties of inorganic flexible materials and their devices reported in the recent 3 years, including sulfides, selenides, tellurides, and composite materials designed based on these inorganics. The structural designs of flexible thermoelectric devices based on micro‐sized bulk materials are also carefully summarized. Additionally, we overview the mechanical stability and methods for reducing internal resistance for designs of inorganic flexible thermoelectric devices. In the end, we provide outlooks on future research directions for inorganic flexible thermoelectric materials and devices. This review will help guide thermoelectric researchers, beginners, and students.
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