Carnot (1796 - 1832)

Carnot discovered that the efficiency of an ideal process depends only on the temperatures.

By brilliant abstract thought the French physicist who developed the theory of heat engines in Réflexions sur la Puissance Motrice du Feu (Reflections on the Motive Power of Fire) (1824) perceived that temperature provided the key.

He realised that the difference in temperature levels is what determines the amount of work that can be obtained from flow of heat. He proposed the reversible Carnot cycle, and discovered that the efficiency of a heat engine depended only on its input and output temperatures.

For Refrigeration, what is the minimum amount of energy necessary to raise the temperature?

Sadi Carnot
Water Wheel

It was known that water flowing from a high level to a low one could do useful work, and the larger the difference in levels, the larger the amount of work.

In those days engineers were beginning to understand steam engines. It was commonly thought that a substance called caloric flowed from the hot substance to the cold one in just the same way as water flows through a water wheel.

Steam Engine

Carnot proposed that work was generated by the passage of caloric from a warmer to a cooler body, with caloric being conserved in the process.

The temperature at which the heat is supplied from the boiler, and that at which heat is rejected in the condenser would be just like the water levels for the water wheel.

Lord Kelvin (1824 - 1907)

Carnot was not completely right, because heat cannot be thought of as a substance which is conserved like Caloric. The same amount of water flows away from a water wheel as enters it. But we now know that less heat flows away from an engine than is put into water in the boiler.

An Englishman called Joule showed what had happened to the lost heat. It had turned into work! This discovery, and the subsequent pioneering work by Clausius in Germany and Thomson (later Lord Kelvin) in Scotland resulted in the Second Law of Thermodynamics, which tells us exactly how much of the heat it is possible to turn into work.

And by implication, this tells us also the minimum amount of work, or power we must put into a refrigerator to make the heat flow from the low temperature level to the high temperature level.

Lord Kelvin