The Carnot Cycle and the Ceiling on Efficiency
A cycle built from two isothermal and two adiabatic legs is the most efficient possible between two temperatures, and its efficiency depends on those temperatures alone. Every real engine is measured against it.
What a learner can do afterwards
- Traces the four legs of the Carnot cycle on a PV diagram and names the heat flow in each
- Computes the Carnot efficiency from the two reservoir temperatures
- Argues why no engine between the same reservoirs can do better
1 · Read
The Carnot cycle runs four reversible legs in order: hot isothermal expansion, adiabatic expansion, cold isothermal compression, and adiabatic compression back to the start. Heat enters only on the hot isotherm and leaves only on the cold one, while the adiabats trade no heat. On a pV plot the enclosed loop area is the work per cycle.
Between 750 K and 300 K the ceiling is one minus 300 over 750, which is 0.60. Between 400 K and 300 K the ceiling is 0.25, so 800 J taken in can give at most 200 J of work. Real stations and fridges are all scored against ceilings like these.
No engine between the same two stores can beat Carnot, because every leg is reversible with no friction or wasted fall. Any challenger leaking extra entropy would need more heat dumped for the same work. Reversible also means the cycle runs backwards as the best refrigerator or heat pump.
Two isotherms plus two adiabats set the ceiling of one minus cold over hot, measured in kelvin.
2 · Watch
Take it off screen
Where it sits
Learn first
This opens up
8 questions wait behind this lesson, each with its answer explained. Every answer feeds the sky: stars light as they are learned, and dim when it is time to come back.