Carnot cycle
- The Carnot cycle is a
theoretical thermodynamic cycle proposed by French physicist
Nicolas Sadi Carnot in 1824.
- It provides an upper limit of
efficiency that any classical thermodynamic engine can achieve during the
conversion of heat into work.
- Conversely, It also provides the efficiency of a refrigeration system in creating a temperature
difference by the application of work to the system.
- It is not an actual thermodynamic
cycle but is a theoretical construct.
- The Carnot cycle consists of an
alternate series of two reversible isothermal processes and two reversible adiabatic processes.
1.
Isothermal expansion process ab: - During the process ab, heat is transferred reversibly
and isothermally to the working substance from the high-temperature reservoir
(HTR) at temperature TH and the system performs an amount of work.
2.
Adiabatic expansion(dc): - During this process (bc), the temperature of the system
decreases from TH to TC.
3.
Isothermal compression process (cd): - During process cd, the system rejects heat Q2
to a low-temperature reservoir (LTR) at a constant temperature TC.
4.
Adiabatic compression: - This is the final step. During this process, the temperature rises from TC to TH and the original
conditions are restored to the system.
- The enclosed area ' abcd '
represents the net work delivered by the engine.
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