Sadi Carnot

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Sadi Carnot was a French engineer (one of the few engineers that history remembers) who contributed greatly to the development of the field of thermodynamics. Although he only published one paper, which went largely unrecognized during his life, a testament to the influence of his ideas is the fact that his ideal heat engine is well known to modern day students of thermodynamics.

Sadi Carnot was born in France in 1796. His life took place during turbulent times; France endured thirty-five years of war, revolution, and unending political turmoil. Twice Napoleon came to power, and twice he was driven out and the monarchy restored. Sadi Carnot's father, Lazare, was one of the most powerful men in France during the early nineteenth century. Not only did he serve as a member of the five-man executive Directory and briefly hold the role of Napoleon's war minister, he also made advancements in science and engineering. Lazare was interested in broad operating principles that govern machinery; his most important conclusion was that accelerations and shocks in the moving parts in machinery must be minimized because they lead to losses of work output.

Although Lazare is most remembered for his work in politics and warfare, his ideas built a foundation for his son Sadi to begin his own work. His work on water machines (such as waterwheels) was particularly influential to Sadi Carnot's thinking; his theoretical heat engine is somewhat analogous to work done when water falls from a high place to a low place.

In 1812, at age 16, Sadi Carnot attended Ecole Polytechnique in Paris. His instructors included Siméon-Denis Poisson, André-Marie Ampère, and François Arago. After graduating, he attended a military engineering school, but later fo...

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... heat pump was less than the work given off by the heat engine (hence the need for a variable work output requirement for this thing to work), then using two differing heat reservoirs you could produce unlimited work.

Carnot was, however, a strong believer in the impossibility of perpetual motion, so he used this whole scenario as proof that there can be no variation in the work output of an ideal heat engine if the heat input Qh and the two reservoir temperatures Th and Tc are the same.

Incidentally, the "heat pump" that Carnot envisioned has a practical application: refrigerators. A refrigerator uses the expansion and compression of a gas to transfer heat away from the inside of the refrigerator and radiate it out to the surroundings. This expansion and compression of the gas requires work to proceed - so the whole process is the opposite of a heat engine.

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