Heat Engine Efficiency Calculator
Find the Carnot efficiency of a heat engine.
Result
How it is calculated
The tool computes the Carnot efficiency η = (1 − Tc / Th) × 100. You type the hot and cold reservoir temperatures in degrees Celsius; the tool first converts them to kelvin with T(K) = T(°C) + 273.15, because the ratio only works on the absolute scale. Th is the hot-side temperature, Tc the cold-side temperature, and the result is a percentage rounded to two decimals.
There is no result if the hot temperature is not higher than the cold one, or if either temperature is below absolute zero (−273.15 °C). The figure is an upper limit set by thermodynamics, not the efficiency of a real engine, which is always lower.
Worked example
A steam plant has a boiler at 500 °C and a condenser at 30 °C. In kelvin: Th = 500 + 273.15 = 773.15 and Tc = 30 + 273.15 = 303.15. The ratio is 303.15 / 773.15 = 0.3921. Then 1 − 0.3921 = 0.6079. The maximum efficiency is 60.79%; no engine working between these two temperatures can beat it.
Common mistakes
- Using Celsius values directly in the ratio by hand (30 / 500); the formula needs kelvin, and the tool adds 273.15 for you, so do not type kelvin values into the Celsius fields.
- Swapping the hot and cold temperatures; the tool then returns nothing because the hot side must be warmer.
- Treating the result as the efficiency a real plant or engine will reach; friction, heat loss and combustion limits push real values well below the Carnot figure.
- Entering the gas or flame temperature of a combustion engine as the hot reservoir when the working fluid actually sees a much lower average temperature.
- Using this for refrigerators or heat pumps; their performance is described by a coefficient of performance, not by this efficiency.
About this calculator
The Carnot efficiency formula η = 1 − Tc/Th (temperatures in Kelvin) gives the theoretical maximum efficiency any heat engine can achieve while operating between a hot reservoir at Th and a cold reservoir at Tc. This limit comes directly from the second law of thermodynamics — no real engine, no matter how well engineered, can exceed it, and every real engine falls further below it due to friction, heat loss, and other irreversibilities.
Mechanical and thermal engineers use this ceiling to benchmark real power plants, internal combustion engines, and refrigeration cycles (which apply the same relationship in reverse) against the best physically possible performance for their operating temperatures. Physics students meet it as the canonical illustration of why perpetual-motion or 100%-efficient engines are impossible.
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