Why is the Carnot Cycle so Important?

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SUMMARY

The Carnot Cycle is crucial in thermodynamics as it establishes the maximum efficiency limit for all reversible engines, defined by the formula 1 - T2/T1. This cycle consists of isothermal and adiabatic processes, making it a standard for demonstrating efficiency. While other cycles, such as those involving isobaric and isochoric processes, can theoretically achieve similar efficiency, they are often less efficient in practice due to irreversibilities. The Carnot Cycle's simplicity and theoretical foundation make it a benchmark for evaluating real engine performance.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically the laws of thermodynamics.
  • Familiarity with the concepts of isothermal, adiabatic, isobaric, and isochoric processes.
  • Knowledge of efficiency calculations in thermodynamic cycles.
  • Basic grasp of entropy and its role in reversible processes.
NEXT STEPS
  • Study the derivation of the Carnot efficiency formula 1 - T2/T1.
  • Explore real-world applications of the Carnot Cycle in heat engines.
  • Investigate the differences between reversible and irreversible processes in thermodynamics.
  • Learn about other thermodynamic cycles, such as the Rankine and Otto cycles, for comparative analysis.
USEFUL FOR

Students and professionals in mechanical engineering, thermodynamics researchers, and anyone interested in the principles of heat engine efficiency.

SUDOnym
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All reversible cyclic processes (engines) have the same efficiency: 1-T2/T1.

And Carnot demostrated this efficiency with the Carnot Cycle and went on to use this to demonstrate that this was the upper limit for efficiency.

My question is, why is it that there is such importance placed on the Carnot Cycle? ie. since all reversible processes have this same efficiency couldn't we say just take an engine whos path is:

a isobaric b isochoric c isobaric d isochoric a isobaric b isochoric c isobaric d isochoric ...and so on.

and use this engine to also demonstrate that the upper limit is 1-T2/T1? is it simply that with the carnot cycle, which is:

a isotherm b adiabat c isotherm d adiabat a isotherm b adiabat c isotherm d adiabat ... and so on

makes it easy to demonstrate this result?
 
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SUDOnym said:
My question is, why is it that there is such importance placed on the Carnot Cycle? ie. since all reversible processes have this same efficiency couldn't we say just take an engine whos path is:

a isobaric b isochoric c isobaric d isochoric a isobaric b isochoric c isobaric d isochoric ...and so on.

and use this engine to also demonstrate that the upper limit is 1-T2/T1? is it simply that with the carnot cycle, which is:

a isotherm b adiabat c isotherm d adiabat a isotherm b adiabat c isotherm d adiabat ... and so on

makes it easy to demonstrate this result?
In order to create a reversible cycle, all heat flow has to occur at infinitessimal temperature differences. In other words, heat flow from the hot reservoir to the system has to occur with the reservoir and system at the same temperature AND heat flow from the system to the cold reservoir has to occur with the system and cold reservoir at the same temperature. In order to get from the hot temperature to the cold temperature and vice-versa without increasing entropy, the expansions and compressions cannot involve heat flow.

So any reversible cycle must be equivalent to the Carnot cycle: isothermal (expansion), adiabatic (expansion), isothermal (compression), adiabatic (compression).

AM
 
SUDOnym said:
My question is, why is it that there is such importance placed on the Carnot Cycle? ie. since all reversible processes have this same efficiency couldn't we say just take an engine whos path is:

a isobaric b isochoric c isobaric d isochoric a isobaric b isochoric c isobaric d isochoric ...and so on.

this cycle is highly irreversible and much less efficient than carnot's cycle
 

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