About the Carnot Efficiency Calculator
This Carnot efficiency calculator gives the theoretical upper limit on how much of the heat flowing from a hot reservoir to a cold one can be turned into work. Enter the hot and cold temperatures in °C, °F or kelvin and it returns the Carnot efficiency, the ideal coefficient of performance (COP) for a refrigerator and a heat pump working between the same temperatures, and — if you give a heat input — the maximum work output and the heat that must be rejected.
Students use it for thermodynamics homework on the second law; engineers and energy enthusiasts use it to sanity-check claims about power plants, engines, solar-thermal systems or heat pumps. No real machine reaches the Carnot limit, so comparing an actual efficiency or COP with the ideal value shows how much room for improvement there is.
The formula only works with absolute temperatures, so the calculator converts everything to kelvin first. The hot reservoir must be hotter than the cold one; if the temperatures are equal, no work can be extracted and the ideal COP becomes unbounded.
With the default inputs, the carnot efficiency is 61.44%. Change any value above to recalculate instantly.
How to use the carnot efficiency calculator
- 1Choose the temperature unit you are working in.
- 2Enter the hot reservoir and cold reservoir temperatures.
- 3Optionally enter the heat input to see the maximum work and rejected heat.
- 4Optionally enter an actual efficiency to compare with the Carnot limit.
- 5Read the efficiency and the ideal COP values.
Formula and method
A Carnot engine is a reversible cycle of two isothermal and two adiabatic steps. Because it generates no entropy, Qc/Qh = Tc/Th, so the fraction of heat converted to work is η = 1 − Tc/Th. Any real engine operating between the same two temperatures is less efficient, which is one statement of the second law of thermodynamics.
Running the cycle backwards gives an ideal refrigerator, whose coefficient of performance is the heat removed per unit work, Tc/(Th − Tc), or an ideal heat pump, which delivers Th/(Th − Tc) units of heat per unit work. Temperatures must be absolute (kelvin); the calculator converts °C with K = °C + 273.15 and °F with K = (°F − 32) × 5/9 + 273.15.
- η
- Carnot (maximum) efficiency
- Th
- Hot reservoir temperature (K)
- Tc
- Cold reservoir temperature (K)
- Qh
- Heat taken from the hot reservoir
- W
- Maximum work output
- COP
- Coefficient of performance
Worked examples
Engine between 500 °C and 25 °C
In kelvin the reservoirs are 773.15 K and 298.15 K, so η = 1 − 298.15/773.15 = 61.44%. From 100 kW of heat, at most 61.4 kW can become work and at least 38.6 kW must be rejected to the cold side.
Heat pump: 35 °C indoor coil, −5 °C outdoors
With Th = 308.15 K and Tc = 268.15 K, the ideal heat pump COP is 308.15/40 = 7.70. Real air-source heat pumps achieve roughly a third to a half of this, but the ideal value shows why smaller temperature lifts give much better COPs.
Steam plant in Fahrenheit running at 40%
1000 °F is 810.93 K and 70 °F is 294.26 K, giving a Carnot limit of 63.71%. A plant running at 40% thermal efficiency therefore achieves about 62.8% of what is theoretically possible.
Frequently asked questions
What is Carnot efficiency?+
It is the highest efficiency any heat engine can reach when operating between two temperatures: η = 1 − Tc/Th with temperatures in kelvin. It is set by the second law of thermodynamics and does not depend on the working fluid.
Why must temperatures be in kelvin?+
The formula depends on the ratio of temperatures, which only has physical meaning on an absolute scale where zero is absolute zero. Using °C or °F directly gives wrong — even negative — efficiencies.
Can an engine be 100% efficient?+
No. Efficiency would only reach 100% if the cold reservoir were at absolute zero, which cannot be attained. Every heat engine must reject some heat to a colder sink.
How is Carnot COP different from efficiency?+
Efficiency measures work out per heat in for an engine and is always below 1. COP measures heat moved per work in for a refrigerator or heat pump and is usually above 1; for a heat pump, COP = 1/η.
How close do real power plants get to the Carnot limit?+
Real cycles lose energy to friction, finite-rate heat transfer and non-ideal components, so they typically reach well under the Carnot figure. The ratio of actual to Carnot efficiency is called the second-law efficiency.