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Mixed/dual cycle

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Thermodynamics
The classical Carnot heat engine
Specific heat capacity  c = {\displaystyle c=} {\displaystyle c=}
T {\displaystyle T} {\displaystyle T} S {\displaystyle \partial S} {\displaystyle \partial S}
N {\displaystyle N} {\displaystyle N} T {\displaystyle \partial T} {\displaystyle \partial T}
Compressibility  β = {\displaystyle \beta =-} {\displaystyle \beta =-}
1 {\displaystyle 1} {\displaystyle 1} V {\displaystyle \partial V} {\displaystyle \partial V}
V {\displaystyle V} {\displaystyle V} p {\displaystyle \partial p} {\displaystyle \partial p}
Thermal expansion  α = {\displaystyle \alpha =} {\displaystyle \alpha =}
1 {\displaystyle 1} {\displaystyle 1} V {\displaystyle \partial V} {\displaystyle \partial V}
V {\displaystyle V} {\displaystyle V} T {\displaystyle \partial T} {\displaystyle \partial T}
  • Internal energy
    U ( S , V ) {\displaystyle U(S,V)} {\displaystyle U(S,V)}
  • Enthalpy
    H ( S , p ) = U + p V {\displaystyle H(S,p)=U+pV} {\displaystyle H(S,p)=U+pV}
  • Helmholtz free energy
    A ( T , V ) = U T S {\displaystyle A(T,V)=U-TS} {\displaystyle A(T,V)=U-TS}
  • Gibbs free energy
    G ( T , p ) = H T S {\displaystyle G(T,p)=H-TS} {\displaystyle G(T,p)=H-TS}

The dual combustion cycle (also known as the mixed cycle, Trinkler cycle, Seiliger cycle or Sabathe cycle) is a thermal cycle that is a combination of the Otto cycle and the Diesel cycle, first introduced by Russian-German engineer Gustav Trinkler, who never claimed to have developed the cycle himself.[1] Heat is added partly at constant volume (isochoric) and partly at constant pressure (isobaric),[2] the significance of which is that more time is available for the fuel to completely combust. Because of lagging characteristics of fuel this cycle is invariably used for Diesel and hot spot ignition engines. It consists of two adiabatic and two constant volume and one constant pressure processes.

Pressure-Volume diagram of Sabathe cycle
Temperature-Entropy diagram of Sabathe cycle

The dual cycle consists of following operations:

  • Process 1-2: Isentropic compression
  • Process 2-3: Addition of heat at constant volume.
  • Process 3-4: Addition of heat at constant pressure.
  • Process 4-5: Isentropic expansion.
  • Process 5-1: Rejection of heat at constant volume.

Bibliography

[edit ]
  • Cornel Stan: Alternative Propulsion for Automobiles, Springer, 2016, ISBN 9783319319308, p. 48

References

[edit ]
  1. ^ Г. В. Тринклер: Двигателестроение за полустолетие. Очерки современника, 2nd edition, Речной транспорт, Saint Petersburg, 1958, p. 32
  2. ^ Lino Guzzella, Christopher Onder: Introduction to Modeling and Control of Internal Combustion Engine Systems, 2nd edition, Springer, Berlin/Heidelberg, ISBN 9783642107757, p. 334


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