The Carnot Engine: Why Nature Puts a Ceiling on Efficiency
Imagine you have a steam engine. You burn coal, heat water, make steam, push a piston. You get work out. But you also always waste heat — the exhaust steam is still hot. Could you ever build an engine that converts all the heat into work? The Carnot engine is the thought experiment that answers that question with a firm no.
The intuition is simple: heat flows spontaneously only from hot to cold. To make it do work, you must let some of it "fall" to a lower temperature, just as a water wheel can only extract work from water falling downhill — you never get all the potential energy back, because the water ends up at the bottom. The Carnot engine is the perfect water wheel: it wastes the absolute minimum heat required by the second law of thermodynamics.
The Precise Definition
A Carnot engine is an idealised, reversible heat engine that operates in a cycle between two thermal reservoirs at temperatures TH (hot) and TC (cold), where TH>TC. The cycle consists of exactly four reversible processes:
- Isothermal expansion at TH — the working substance (usually an ideal gas) absorbs heat QH from the hot reservoir while expanding slowly, doing work on the surroundings.
- Adiabatic expansion — the gas is thermally insulated and continues expanding, doing work. Its temperature drops from TH to TC with no heat exchange.
- Isothermal compression at TC — the gas is in contact with the cold reservoir. It is compressed slowly, rejecting heat QC to the cold reservoir.
- Adiabatic compression — the gas is insulated again and compressed further, raising its temperature back to TH with no heat exchange, returning to the starting state.
Every step is reversible — the gas is always in thermodynamic equilibrium, and the direction can be reversed by an infinitesimal change. This is the ideal limit that real engines can approach but never reach.
The Efficiency — The One Result You Must Know
The efficiency η of any heat engine is defined as:
η=Heat inputWork output=QHW
From energy conservation over one cycle, W=QH−QC, so:
η=1−QHQC
For a Carnot engine, the ratio of heat exchanged is exactly equal to the ratio of absolute temperatures:
QHQC=THTC
ηCarnot=1−THTC
This is the maximum possible efficiency for any engine operating between TH and TC. No real engine can beat it — not because of engineering limitations, but because of the second law of thermodynamics.
Temperatures must be in Kelvin. Using Celsius gives a completely wrong (and often >1) result. For example, between 100°C and 0°C, TH=373K, TC=273K, so η=1−273/373≈0.27 (27%). If you used Celsius, you'd get 1−0/100=1 (100%), which is impossible.
Why This Is the Maximum …
