Carnot Efficiency Calculator
Find the maximum possible (Carnot) efficiency of a heat engine from its hot and cold reservoir temperatures, η=1-Tc/Th.
🔥 What is the Carnot Efficiency Calculator?
This Carnot efficiency calculator finds the theoretical maximum efficiency of a heat engine from η=1−Tc/Th. Enter the hot and cold reservoir temperatures in Kelvin, and it returns the maximum possible efficiency as a percentage.
With Th=600 K and Tc=300 K, this calculator gives exactly 50% efficiency, a classic textbook benchmark.
No real engine can exceed this limit, and no real engine actually reaches it, the Carnot efficiency is an absolute ceiling set by the second law of thermodynamics, independent of the engine's design or working fluid.
This calculator is useful for thermodynamics students and engineers evaluating the theoretical performance ceiling of heat engines, power plants, and turbines.
📐 Formula
📖 How to Use This Calculator
Steps
💡 Example Calculations
Example 1 - Classic textbook benchmark
Example 2 - Higher boiler temperature power plant
Example 3 - Boiling water to room temperature
❓ Frequently Asked Questions
🔗 Related Calculators
What is Carnot efficiency?
Carnot efficiency is the theoretical maximum efficiency any heat engine can achieve while operating between a hot reservoir at temperature Th and a cold reservoir at temperature Tc, given by η=1−Tc/Th. It is an absolute upper bound set by the second law of thermodynamics, not by any particular engine design.
What is the formula for Carnot efficiency?
η = 1 − Tc/Th, where Th and Tc are the absolute (Kelvin) temperatures of the hot and cold reservoirs respectively. Both temperatures must be in Kelvin, not Celsius or Fahrenheit, for the formula to give a correct result.
Why must temperatures be in Kelvin for this formula?
The Carnot formula derives from the thermodynamic (absolute) temperature scale, where zero represents absolute zero. Using Celsius or Fahrenheit directly (where zero is arbitrary) gives an incorrect ratio and a wrong efficiency value.
Can any real engine reach Carnot efficiency?
No, the Carnot efficiency assumes a perfectly reversible process with no friction, no irreversible heat transfer, and infinitely slow (quasi-static) operation, conditions no real engine can achieve. Carnot efficiency is a theoretical ceiling that real engines can only approach, never reach.
Why does a wider temperature difference give higher efficiency?
Since η=1−Tc/Th, increasing Th or decreasing Tc directly increases efficiency, this is exactly why power plant designers push for the highest practical boiler/turbine inlet temperature and seek the coldest available cooling source (like river or seawater) to maximize the temperature gap.
What is a real-world example of Carnot efficiency in use?
A power plant with a boiler at 600 K (327°C) rejecting heat to a river at 300 K (27°C) has a maximum possible Carnot efficiency of 50%, meaning even a perfect engine could convert at most half the input heat into useful work, real plants achieve considerably less due to practical losses.
Is Carnot efficiency the same for any working fluid (steam, gas, etc.)?
Yes, remarkably, Carnot's theorem proves that the maximum efficiency between two given temperatures depends only on those two temperatures, not on the working substance or the specific engine design, a landmark result in thermodynamics.
What happens to Carnot efficiency as the cold reservoir approaches absolute zero?
As Tc approaches 0 K, Carnot efficiency approaches 100% (η→1). In practice, absolute zero is unreachable (third law of thermodynamics), so 100% efficiency is never actually achievable.
How does Carnot efficiency relate to refrigerators and heat pumps?
The same Carnot cycle run in reverse sets the maximum theoretical coefficient of performance (COP) for refrigerators and heat pumps operating between the same two temperatures, a closely related but differently expressed quantity from engine efficiency.
Why is Carnot efficiency important even though it's unachievable?
It provides an absolute benchmark for judging how much theoretical room for improvement exists in a real engine or power plant design, engineers compare actual efficiency against the Carnot limit to gauge how close a design comes to the physical maximum.