Thermoelectric energy conversion: Conversion of heat into electrical energy or vice versa

Temperature gradient creates a potential difference.

Temperature gradient creates a potential difference.

Connecting the 2 ends via an electrical conductor results in a current flow.

Connecting the 2 ends via an electrical conductor results in a current flow.

Thermoelectrics are materials which are capable of converting heat into electrical energy and vice versa. This fascinating phenomenon is nowadays commercially used in power generators (e.g., in the telecommunication industry, or in spacecrafts), food refrigerators, air conditioning, cryotherapy, pacemakers, and sensors (e.g. thermocouples). The automobile industry is eager to use this technique, e.g. for environmentally harmless air conditioning or as a power source for the radio or headlights, driven by the exhaust heat. The applications are to date limited due to the somewhat low efficiency η (ca. 5% - 10%):


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Formulae for efficiency and figure-of merit

Efficiency formula and figure-of-merit

Typical values might be TH = 800°C, TC = 400°C, zT = 1, yielding a theoretical η = 7.6%. The peak figure-of-merit is close to 1 in the materials commercially used. The Seebeck coefficient α and the electrical conductivity σ can be measured using our ZEM-3 M-8 (ULVAC-RIKO), and the thermal conductivity κ can be determined with our DLF-1 (TA Instruments).

DLF-1 (TA Instruments) in the lab.
DLF-1 (TA Instruments) in lab.

An increase of zT by a factor of two or more would be necessary to become competitive to Freon compressors as used in conventional refrigerators.

The best thermoelectric materials exhibit an intermediate charge carrier concentration (e.g., doped small band-gap semiconductors), a high mobility of the charge carriers (achieved by using elements with similar electronegativities) and low thermal conductivity, which can be reached by using heavy elements, mixed occupancies, rattling of atoms, and low-symmetry structures.

To improve on these characteristics is the ultimate goal in our research group.

Figure of merit versus temperature for four materials.

Temperature dependence of the thermoelectric figure-of-merit of environmentally benign materials (own research).

Recommended references

  • H. R. Freer, A. V. Powell,ÌýJ. Mater. Chem. CÌý8, 441 (2020):
    ÌýÌýfuture opportunities for thermoelectric materials.Ìý
  • Y. Shi, C. Sturm, H. Kleinke,ÌýJ. Solid State Chem.Ìý270, 273 (2019):
    ÌýÌýaÌýreviewÌýcovering various chalcogenides for power generation.
  • X. Cheng, N. Farahi, H. Kleinke,ÌýJOMÌý68, 2680 (2016):
    ÌýÌýaÌýreviewÌýcovering environmentally benignÌýMg2SiÌýmaterials for power generation.
  • H. Kleinke,ÌýChem. Mater.Ìý22, 604 (2010):
    ÌýÌýaÌýreviewÌýcovering advanced thermoelectric materials for power generation.
  • N. K. Barua, E. Hall, Y. Cheng, A. O. Oliynyk, H. Kleinke,ÌýChem. Mater. 36, 7089 (2024):
    Ìý machine learning to predict thermal conductivity.
  • C. Gayner, L. T. Menezes, Y. Natanzon, Y. Kauffmann, H. Kleinke, Y. Amouyal, ACS Appl. Mater. Interf. 15, 13012 (2023):
    Ìý scalable solution synthesis of nanostructured Bi2Te3.
  • D. C. Ramirez, L. R. Macario, X. Cheng, M. Cino, D. Walsh, Y.-C. Tseng, H. Kleinke,ÌýACS Appl. Energy Mater.Ìý3, 2130 (2020):
    ÌýÌýupscaling the synthesis of environmentally friendly thermoelectric materials.
  • P. Jafarzadeh, M. Oudah, A. Assoud, N. Farahi, E. Müller, H. Kleinke,ÌýJ. Mater. Chem. CÌý6, 13043 (2018):
    ÌýÌýnew copper sulfide-tellurides with highÌýzTÌýand good stability.
  • Y. Shi, A. Assoud, S. Ponou, S. Lidin, H. Kleinke,ÌýJ. Am. Chem. Soc.Ìý140, 8578 (2018):
    ÌýÌýthe first composite structure withÌýzTÌýabove unity.
  • N. Farahi, S. Prabhudev, G. A. Botton, J. R. Salvador, H. Kleinke,ÌýACS Appl. Mater. InterfacesÌý8, 34431 (2016):
    ÌýÌýnano- and microstructure engineering enhancesÌýzTÌýto 1.4 for Bi-dopedÌýMg2(Si,Sn).
  • Q. Guo, A. Assoud, H. Kleinke,ÌýAdv. Energy Mater.Ìý4, 1400348 (2014):
    ÌýÌýTl10-δSnδTe6Ìýand Tl10-δPbδTe6ÌýexceedÌýzTÌý= 1.