Skip to main content

Finite Time Thermodynamic Analysis of Stirling and Ericsson Power Cycles

  • Chapter
  • First Online:
Finite Time Thermodynamics of Power and Refrigeration Cycles

Abstract

In 1816, Robert Stirling and James Stirling conceived and patented an external combustion heat engine, which turned by their name and was continuously improved by them over the next 30 years. It is also a reversible cycle like the Carnot cycle and, hence, also has the highest thermal efficiency working between two (high and low) temperatures of source and sink reservoirs, but it has some advantages over the Carnot cycle. The Stirling heat engine consists of two cylinders with two pistons on each side and a regenerator in the middle, which is used for temporary storage of thermal energy. The Stirling engine is a closed system and also required more innovative hardware for execution. In 1833, the Swedish-born engineer John Ericsson developed a different type of hot air, reciprocating, external combustion engine, which could operate on either an open or closed loop cycle.

This is a preview of subscription content, log in via an institution to check access.

Access this chapter

Institutional subscriptions

References

  • Badescu, V. (1992). Optimum operation of solar convertor in combustion with a Stirling or Ericsson heat engine. Energy, 17, 601–607.

    Article  Google Scholar 

  • Blank, D.A., Davis, G.W. and Wu, C. (1994). Power optimization of an endoreversible Stirling cycle with regeneration. Energy, 19, 125–133.

    Article  Google Scholar 

  • Blank, D.A. and Wu, C. (1995). Power optimization of an extra-terrestrial solar radiant Stirling heat engine, Energy, 20(6), 523–530.

    Article  Google Scholar 

  • Blank, D.A. and Wu, C. (1996a). Power limit of an endoreversible Ericsson cycle with regeneration. Energy Convs. Mgmt, 37, 59–66.

    Article  Google Scholar 

  • Blank, D.A. and Wu, C. (1996b). Finite time power limit for solar-radiant Ericsson engines for space applications. Applied Thermal Engineering, 18, 1347–1357.

    Article  Google Scholar 

  • Chen, J. (1997a). Optimal performance analysis of irreversible cycles used as heat pumps and refrigerators. J. Phys. D: Appl. Phys, 30, 582–587.

    Article  ADS  Google Scholar 

  • Chen, J. (1997b). Effect of regenerative losses on the efficiency of Stirling heat engine at maximum power output. Int. Journal of Ambient Energy, 18, 107–112.

    Article  Google Scholar 

  • Chen, J. and Schouten, J.A. (1999). The comprehensive influence of several major irreversibilities on the performance of an Ericsson heat engine. Applied Thermal Engineering, 19, 555.

    Article  Google Scholar 

  • Chen, J., Yan, Z., Chen, L. and Andresen, B. (1998). Efficiency bound of solar-driven Stirling heat engine system. Int. Journal Energy Res, 22, 805–812.

    Article  Google Scholar 

  • Curzon, F.L. and Ahlborn, B. (1975). Efficiency of a Carnot engine at maximum power output. American Journal of Physics, 43, 22–24.

    Article  ADS  Google Scholar 

  • Erbay, L.B. and Yavuz, H. (1997). Analysis of Stirling heat engine at maximum power conditions. Energy, 22, 645–650.

    Article  Google Scholar 

  • Kaushik, S.C. (1999). State-of-the-art on finite time thermodynamics. Internal Report CES, IIT Delhi, India.

    Google Scholar 

  • Kaushik, S.C. and Kumar, S. (2000a). Finite time thermodynamic analysis of an endoreversibble Stirling heat engine with regenerative losses. Energy, 25, 989–1003.

    Article  Google Scholar 

  • Kaushik, S.C. and Kumar, S. (2000b). Finite time thermodynamic evaluation of irreversible Ericsson and Stirling heat pump cycles, Proceedings of 4th Minsk International Seminar on Heat Pipes, Heat Pumps & Refrigerators, Minsk, Belarus 2000b, 113–126.

    Google Scholar 

  • Kaushik, S.C. and Kumar, S. (2001). Finite time thermodynamic evaluation of irreversible Ericsson and Stirling heat engines. Energy Convers. Mgmt, 42, 295–312.

    Article  Google Scholar 

  • Kaushik, S.C. and Tyagi, S.K. (2002). Finite time thermodynamic analysis of a nonisentropic regenerative Brayton heat engine. Int. J. Solar Energy, 22, 141–151.

    Google Scholar 

  • Kumar, S. (2000). Finite time thermodynamic analysis and second law evaluation of thermal energy conversion systems. Ph.D. Thesis, C.C.S. University, Meerut India.

    Google Scholar 

  • Ladas, H.G. and Ibrahim, O.M. (1994). Finite time view of Stirling heat engine. Energy, 19, 837–843.

    Article  Google Scholar 

  • Senft, J.R. (1998). Theoretical limits on the performance of Stirling engine. Int Journal Energy Res, 22, 991–1000.

    Article  Google Scholar 

  • Trukhow, V.S., Tursunbaev, I.A., Lezhebokov, I.A. and Kenzhaev, I.G. (1997). Energy balance of autonomous solar power plant, with the Stirling engine Appl Solar Energy, 33, 17–23.

    Google Scholar 

  • Tyagi, S.K., Kaushik, S.C. and Salhotra, R. (2002). Ecological optimization and parametric study of irreversible Ericsson and Stirling heat engines. Journal of Phys D: Appl. Phys, 35, 2668–2675.

    Article  ADS  Google Scholar 

  • Zhou Yinghui, Tyagi S. K., and Chen J., The optimal performance of an irreversible Braysson heat engine cycle, Int. Journal of Thermal Sciences, Vol.43 (2004) pp.1101–1106.

    Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

Copyright information

© 2017 Capital Publishing Company, New Delhi, India

About this chapter

Check for updates. Verify currency and authenticity via CrossMark

Cite this chapter

Kaushik, S.C., Tyagi, S.K., Kumar, P. (2017). Finite Time Thermodynamic Analysis of Stirling and Ericsson Power Cycles. In: Finite Time Thermodynamics of Power and Refrigeration Cycles. Springer, Cham. https://doi.org/10.1007/978-3-319-62812-7_6

Download citation

Publish with us

Policies and ethics