2016
DOI: 10.1016/j.rser.2016.06.035
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A review on nanostructures of high-temperature thermoelectric materials for waste heat recovery

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Cited by 300 publications
(115 citation statements)
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“…The radiation spectrum of thermophotovoltaic emitter has to be matched with the bandgap of the photovoltaic cell, which generally requires the emitter temperature to be at least 730 °C (1000 K) for practical power density and conversion efficiency. While thermoelectric devices have been used at room and moderate temperatures for refrigeration and waste heat recovery, there is continued push for high‐efficiency thermoelectric materials at high temperature, such as Si–Ge, half‐Heusler, and oxides, for applications in space exploration, high‐temperature waste heat harvesting (e.g., from industrial furnaces), and combustion‐ or solar‐driven generators 14a…”
Section: Introductionmentioning
confidence: 99%
“…The radiation spectrum of thermophotovoltaic emitter has to be matched with the bandgap of the photovoltaic cell, which generally requires the emitter temperature to be at least 730 °C (1000 K) for practical power density and conversion efficiency. While thermoelectric devices have been used at room and moderate temperatures for refrigeration and waste heat recovery, there is continued push for high‐efficiency thermoelectric materials at high temperature, such as Si–Ge, half‐Heusler, and oxides, for applications in space exploration, high‐temperature waste heat harvesting (e.g., from industrial furnaces), and combustion‐ or solar‐driven generators 14a…”
Section: Introductionmentioning
confidence: 99%
“…Thermoelectric materials show great potential application in the field of waste heat recovery, power generators and solid refrigeration due to their direct conversion between heat energy and electrical energy. The conversion efficiency of thermoelectric material is primarily governed by the dimensionless figure-of-merit, ZT = α 2 σT/(κ L + κ e )κ, where α, σ, α 2 σ, κ L , κ e and T are the Seebeck coefficient, electrical conductivity, power factor, lattice thermal conductivity and carrier thermal conductivity of total thermal conductivity κ and absolute temperature, respectively [1][2][3]. As the physical parameters α, σ, and κ e are coupled via effective mass (m*) and carrier concentration (n), it is a major challenge to improve the ZT by independently optimizing these parameters.…”
Section: Introductionmentioning
confidence: 99%
“…The expected decrease of κ L due to the addition of nano-TiO 2 is not evident in other TiO 2 /Cu 2 SnSe 3 composites, which is possibly attributed to the distribution of nano-TiO 2 in the grain boundaries. However, the κ L of 1.4%TiO 2 Cu2SnSe3 sample, the lower κL of TiO2/Cu2SnSe3 sample in this study should be related with the distribution of TiO2. Figure 10 shows the temperature dependence of the dimensionless figure of merit ZT of TiO2/Cu2SnSe3 composites.…”
Section: Resultsmentioning
confidence: 54%
“…In the process of industrial production, most energy is released in the form of heat. Thermoelectric (TE) materials can directly convert waste heat into electricity based on the Seebeck effect [1,2]. While TE materials show a great prospect environmentally and economically, the lower efficiency of TE materials limits their wide application.…”
Section: Introductionmentioning
confidence: 99%