Electrically tunable thermal conductivity in thermoelectric materials: Active and passive control

Applications involving the use of thermoelectric materials can be found in many different areas ranging from thermocouple sensors, portable coolers, to solar power generators. Generally, they can be subdivided by the direction of energy conversion. While the Peltier effect is used in solid-state ref...

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Detalles Bibliográficos
Autores: Massaguer Colomer, Albert, Massaguer Colomer, Eduard, Pujol i Sagaró, Toni, Comamala Laguna, Martí, Montoro Moreno, Lino, González Castro, Josep R.
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2015
País:España
Institución:Varias* (Consorci de Biblioteques Universitáries de Catalunya, Centre de Serveis Científics i Acadèmics de Catalunya)
Repositorio:Recercat. Dipósit de la Recerca de Catalunya
OAI Identifier:oai:recercat.cat:10256/12202
Acceso en línea:http://hdl.handle.net/10256/12202
Access Level:acceso embargado
Palabra clave:Materials termoelèctrics
Thermoelectric materials
Termoelectricitat
Thermoelectricity
Conductivitat tèrmica
Descripción
Sumario:Applications involving the use of thermoelectric materials can be found in many different areas ranging from thermocouple sensors, portable coolers, to solar power generators. Generally, they can be subdivided by the direction of energy conversion. While the Peltier effect is used in solid-state refrigeration, the Seebeck effect is responsible for the conversion of temperature gradients into electrical voltage in energy harvesting systems. However, this paper proposes a novel approach to the use of thermoelectric couples, treating them as variable insulators in thermal systems. Here, we demonstrate that thermal conductivity in thermoelectric materials can be externally controlled by electrical parameters such as electrical load or DC voltage in passive and active systems, respectively. Active mode is a good solution when a complete insulation or a high control of thermal conductivity is needed. Passive mode permits a thermal conductivity increment of 1. +. ZTtimes with respect to semiconductor initial thermal conductivity. Results open new doors and new opportunities for thermoelectric materials