The operation of a thermoelectric cell can be described schematically by analogy with an enclosure containing a thermodynamic working fluid. In this case, the working fluid is the electron gas, which can be likened to a perfect gas. The condition of a perfect gas is understood here as that of a gas with no interaction between particles, with the exception of elastic collisions, which ensure a microscopic velocity distribution compatible with the definition of a temperature, i.e. a stable thermal velocity spectrum. The electrochemical electron potential μ takes the place of the partial pressure for the electron gas. We can then write:
You do not have access to this resource.
Exclusive to subscribers. 97% yet to be discovered!
(1) - ROWE (D.M.) Éd -
CRC Handbook of thermoelectrics : macro to nano.
-
RC : Boca Raton, FL, USA (2006). SEEBECK (T.J.). – Ueber den magnetismus der galvanischen kette. Technical report for the Royal Prussian Academy of Science, Berlin, Germany (1821).
(2) -...
You do not have access to this resource.
Exclusive to subscribers. 97% yet to be discovered!
This offer includes interactive articles. Their quizzes highlight the key information to remember and validate their acquisition: from reader to player, you can enrich your knowledge.
You can easily identify them thanks to this pictogram: