Why Do Different Methods Yield Different Efficiencies in a Reversible Cycle?

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SUMMARY

The discussion centers on the efficiency of a reversible cycle involving a monoatomic ideal gas, specifically addressing discrepancies in efficiency calculations using two methods. The Carnot theorem establishes that all reversible machines operating between two temperatures have the same efficiency, yet the example presented shows an efficiency of 0.12 when calculated as work over absorbed heat, versus 0.25 using the formula 1-Tc/Th. The key reason for this difference is that the isochoric process introduces heat at intermediate temperatures, reducing overall efficiency compared to cycles where heat is transferred solely at the maximum temperature.

PREREQUISITES
  • Carnot theorem and its implications on reversible cycles
  • Understanding of isochoric, adiabatic, and isothermal processes
  • Basic thermodynamic principles related to ideal gases
  • Efficiency calculations in thermodynamic cycles
NEXT STEPS
  • Study the derivation and implications of the Carnot theorem
  • Explore the characteristics of isochoric and adiabatic processes in depth
  • Learn about the efficiency of various thermodynamic cycles, including Rankine and Otto cycles
  • Investigate the impact of heat transfer at different temperatures on cycle efficiency
USEFUL FOR

This discussion is beneficial for students and professionals in thermodynamics, mechanical engineers, and anyone interested in optimizing the efficiency of thermodynamic cycles.

L0r3n20
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I just read about Carnot theorem (the highest efficiency is the one of reversible machines and all reversible machines working between two given temperatures have the same efficiency).

Then I found a problem where I have a reversible cycle made of an isochoric, adiabatic and isotherm. I report here the data. Computing the efficiency as work/absorbed heat I get 0.12 while if I use 1-Tc/Th I have 0.25. Why are the twos not the same?

The problem states:
"A monoatomic ideal gas is in a state A where the temperature is 300K, p= 2atm and V = 20L. Through an isochoric process the temperature rise up to 400K (state B); through an adiabatic process the gas arrive in a state C where Tc = Ta = 300K and finally through an isotherm process it gets back to A. Compute the efficiency of the cycle.
 
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Good question. When people say that "all reversible engines working between two given temperatures have the same efficiency", they are talking about cases where heat is transferred to or from the engine only at the two given temperatures. In the example with the isochoric process, the temperature of the engine will continuously increase as heat is added during the isochoric process. So, the engine will take in heat at temperatures intermediate between the two given temperatures. This cycle has less efficiency compared to a cycle where all of the heat is added at the highest given temperature.
 
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Thanks! That's exactly what I needed To understand!
 

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