## First Law of Thermodynamics: History of the Concept of Energy

The first law of thermodynamics is basically as follows: there are different types of energy, the energy of motion, the energy in a compressed spring, the energy of rock lifted off the ground, the energy of heat, nuclear energy, etcetera.  Energy can be transferred from one type to another and from one object to another, but the grand total is always the same, where the work (the force times the distance) equals the change in energy of a single object.  This law didn’t, as Marie Slodowska Curie likes to say, spring fully armed from Jupiter’s head like Minerva, but instead was the product of dozens of people debating the nature of force, heat, and motion for over 150 years!  Ready to learn the story? Let’s go!

While researching how destructive sunlight could be if it had mass Emilie started to study what different scientists thought about the damaging effect of moving objects.  Of course, having just co-written a book on Newton, she was aware of Newton’s view on matter and force.  However, despite what I was told in school, Newton never wrote that force equals mass times acceleration.  In fact, the closest he came to it was, “a change in motion is proportional to the motive force impressed[4].”  Instead, Newton was focused on mass times speed as if two objects collided with identical mass times speed and stuck they would stop moving (for this reason, some people started calling mass times to speed the “deadly force”).  However, unlike most French and English scientists at the time, Emilie du Chatelet wasn’t limited to Newton.  See, at the time, science was almost a nationalist pastime.  If you were English, you needed to support Newton, if you were German, Leibnitz, if French, Descartes often to the exclusion of the others.  Emilie thought that was ridiculous and wrote, “About a book of physics one must ask if it is good, not if the author is English, German, or French.”  Or as Voltaire put it, “in the kingdom of Madame du Chatelet, there is absolute freedom of conscience.[5]”  In 1738 or so Emilie learned that a few years before Newton, Newton’s rival Gottfried Leibniz proposed something he called the living force that was dependent on the mass times the velocity squared which was conserved when objects bounced off each other (living because this “force” was only conserved for moving objects).  Newton and Leibniz were enemies and had long arguments about who discovered Calculus so that almost everyone in Europe was firmly in one camp or the other.  However, Emilie felt differently telling her son, “do not carry respect for the greatest men to the point of idolatry… no book is so good that one might not improve it.”  One of the definitive experiments that convinced Emilie du Chatelet that the damage from stopping a moving object is related to the mass times the speed squared (or the “living force”) is dramatized in the 2005 documentary “Einstein’s Big Idea”:

Anyway, in 1740, Emilie du Chatelet published a book called “Lessons in Physics” which was the first to champion Newton’s theories and the idea of living force and helped promote both Newton’s and Liebniz’s theories in France, Germany, and even England.  One reviewer gushed, “there appeared at the beginning of this year a work that would give honor to our century if it were by one of the principal members of the Academies of Europe.  This work, however, is by a woman, [who] has had for a teacher only her genius and her application to self-instruction.”  Du Chatelet continued to research science and by 1747, du Chatelet started to work on her magnum opus, the first French translation of Newton’s Principia with footnotes about the living force.  Tragically, she died just before its publication at age 42 from complications from childbirth.  After her death, Emilie du Chatelet’s ideas about Newton, Leibniz, fire, light, philosophy, and living forces, were all reproduced (sometimes plagiarized word for word) by her friend Diderot in the very influential French Encyclopedia.  Her influence was obscured by her death, but her scientific theories flourished.

Fast forward to England in 1807.  That was when a doctor and scientist named Thomas Young, who was famous for his double-slit experiment from a few years earlier that demonstrated that light acts like a wave, was asked to give a series of talks on the current state of the science.  Young decided to make his talks as simple as possible as his lectures were devoted to the women in the audience as he thought “the acquisition of knowledge” was superior to “the insipid consumption of superfluous time”.  Anyway, in his fifth lecture (out of 60) Young decided that rename the living force (the mass times the speed squared) saying that “the living force … is somewhat more concisely expressed by the term energy”.  Young’s lectures were published as a book and his simplified physics “for the ladies” became a popular science textbook in the 1800s.  Soon, the term “energy” for mass times speed squared started to gain popularity although only in England.

Now we go back to France (again) and two ex-soldiers, Sadi Carnot and Gasbard-Gustave Coriolis, who were interested in the efficiency of machines.  As Carnot put it, “the study of engines is of the greatest interest, [as] their importance is enormous… and they seem destined to produce a great revolution in the civilized world.[6]”  Both men were children of soldiers who went to the same school to become engineers for the military in the very early 1800s.  However, Carnot started in a far better position in French society as he was the son of one of Napoleon’s top captains and Coriolis was the son of one of the former King’s top captains, and King Louis the 16th had been decapitated when Coriolis was just an infant.  They switched social positions in 1815 when Napoleon was defeated (again) and Carnot’s father was exiled.  Sadi Carnot was allowed to remain but generally found military life frustrating with no family power.  By 1818 Carnot left the military and holed up in his brother’s apartment in Paris secretively studying science (Carnot wouldn’t even tell his brother what he was working on).  Meanwhile, Coriolis’s father died and Coriolis dropped out of the army to make a little more money as a scientist studying mechanical systems.  Because of his engineering background, Coriolis had far more technical expertise in machines than the typical academic and in 1829 Coriolis published a book on the physics of machines.  In this book, Coriolis defined a new term that he called work defined as the force times the distance in the direction of motion.  Surprisingly, this is still the modern definition of Work.  Moreover, with this new definition of Work, Coriolis used calculus and found that if an object was pushed on a flat surface the object would have a change in ½ the mass times the speed squared.  He, therefore, decided to make a “slight modification[7]” to the definition of the “living force” and define it as ½ mv^2 (instead of mv^2) to add “simplicity to the principles[8]”.  He then found that if you had a machine that pushed an object up a hill then the Work minus the weight times the height equaled the change in “living force”.  In other words, the work equals the change in the potential energy due to gravity (mgh) plus the change in kinetic energy (1/2mv^2).  If this sounds like what you learned in High School Physics you are right!  The only thing missing was the heat.

Now we go back to Carnot hiding out in his brother’s apartment.  In 1824, Carnot decided to publish his theories on heat and heat engines.  In this pamphlet, Carnot assumed that heat came from hot objects and went to cold objects, and the bigger the temperature difference, the more efficient the engine (all things we consider true today).  Carnot then came up with the form of an idealized engine that would be the most efficient (the Carnot engine).  He then declared that “the production of … power is not …[due] to the actual consumption of [heat], but to its transportation from a warm body to a cold body.[9]”  In other words, Carnot thought that heat engines absorb the same amount of heat that they discharge and it is the movement of heat that allows the engine to perform work.  (The theory that heat is a fluid that is always conserved was called the caloric theory and was very popular in France at the time.)  Over the years, Carnot privately started to rethink the idea of heat as an indestructible fluid.  He wrote in his notebook, “When a hypothesis no longer suffices to explain phenomena, it should be abandoned.  This is the case with regards [to the imperishable] caloric.[10]”  In around 1830 or so Carnot prophetically wrote, “Heat is simply… a movement among the particles of bodies.  Wherever there is the destruction of motive power there is, at the same time, production of heat in quantity exactly proportional to the quantity of motive power destroyed.  Reciprocally, wherever there is the destruction of heat, there is the production of motive power.[11]”  Tragically, before he could publish these thoughts Carnot died of Cholera (at the age of 36) and his private words were only published in 1890, many years after others gained fame for their discovery.  Very few people read Carnot’s work while he was alive, but 2 years after his death another Frenchman and engineer named Paul Clapeyron used it for his book on heat engines which slowly gained popularity around the world.

Whew!  That is a lot of people, let’s do a little recap.  In 1747 Emilie du Chatelet combined the ideas of conserving “living force” (mv^2) with Newton’s ideas and her theories were plagiarized/ ahem memorialized in the French Encyclopedia of 1751.  In 1807, Robert Young gave a series of lectures “for the ladies” where he renamed the “living force” the “energy”.  In 1824, Carnot wrote his book on heat.  In 1827 Coriolis defined Work as Force times distance and redefined the “living force” (ie. kinetic energy) as ½ mv2.  In 1834 Clapeyron published his thoughts on Carnot’s work including the idea that heat flows from hot to cold and the erroneous idea that heat is indestructible.

Now we move back to England and a young brewer named James Joule.  In 1840, 22-year-old Joule decided to systematically study if an electric motor would be more efficient than a steam engine in his bottling factory.  Joule then found an equation for the amount of heat that a resistor would produce and created an equation we still use today (P = I^2R).  He also studied how much chemical energy was used in the battery and was surprised to find the equivalent.  Joule became fascinated with the science and started building elaborate (and astonishingly precise) devices where falling weights would drive a spinning paddle, which would then increase the temperature of the water to demonstrate the relationship between work and heat.   By 1843, Joule was trying to convince anyone and everyone that, “wherever mechanical force is expended, an exact equivalent of heat is always obtained.”  But Mr. Joule was not a professor, just a lowly brewer, so he was mostly ignored, but he kept on speaking wherever anyone would listen.

Clausius was born in 1822 and was the youngest of 18 children!  Yep, I said that right 18.  When Clausius was 21, his family ran into financial difficulties and he ended up working as a high school teacher while he got his Ph.D.  (Clausius remained a devoted teacher his entire life and even gave lessons on his deathbed).  When 26-year-old Clausius read Thomson’s papers he was intrigued and felt that it might be a way to make his name and get out of teaching high school.  Like Emilie du Chatelet over 100 years before, Clausius took what seemed like desperate and conflicting ideas and elegantly meshed them together.  In 1850, Clausius then came up with a new theory that was “opposed, not to the real fundamental principle of Carnot, but to the addition ‘no heat is lost”.  Clausius wrote that Carnot’s theories and heat being a form of energy, “may not only exist together but that they mutually support each other”.  Clausius included the idea of what he called “interior work” (as compared to “exterior work”).   This interior work, which he gave the letter U, represented how the heat affected the internal heat of the gas or changed its properties.   We know to call the “interior work” the internal energy although we still use the letter U.   In fact, one of the modern forms of the first law, is that the change in internal energy equals the heat added minus the work done by an object is exactly how Clausius put it, with the same sign conventions, AND the same letters used!   With this paper, Clausius made his mark in the scientific world and finally got a job as a professor.

Meanwhile, Thomson said that he independently realized that Clausius was right in that Heat is not conserved but energy is.  Thomson then published a series of five papers “On the Dynamical Theory of Heat” between 1851 and 1855 where he lay out new mathematics and theories on the conservation of energy.  In these papers, Thomson used the term energy instead of “living force”.  In 1852, Thomson divided energy into two types, “statical and dynamical” which was very good entomology in my humble opinion.  However, another Scottish scientist, William Rankine, named it “potential and actual” in 1853, and then Thomson changed it to “potential and kinetic” in 1855, the names we are stuck with today.  Although Clausius had innumerable petty arguments with Thomson, he decided that the term “energy” was appropriate as “an abbreviated mode of expression,” and by 1865 Clausius had formed the first law to be that: “the energy of the universe is constant”.  As Richard Feynman said, “conservation of energy… is a most abstract idea, because… it is not a description of a mechanism or anything concrete; it is just a strange fact that we can calculate some number and when we finish watching nature go through her tricks and calculate the number again, it is the same.”  But as a mathematical trick it sure is powerful.  In 1881, Thomson wrote, “the very name energy, … first used in its present sense by Dr. Thomas Young [is now] a principle pervading all nature and guiding the investigator in every field of science.[15]

Clausius wasn’t done yet and in 1854 Clausius came up with a new, second law.  This law was about the heat over the temperature.  Clausius stated that for a perfect reversible cycle the heat divided by the temperature for the full cycle would add to zero and for anything else this quantity would be positive.  By 1865, Clausius renamed this function the “entropy” of a system and wrote the second law to be “the entropy of the universe is increasing”.  But what is entropy, why did he name it that, what does it mean and what does it mean about the universe?  That is next time on the Lightning tamers!

Clausius began to study different processes for a heat engine and determined that if two processes were equivalent, then the heat over the temperature had to be the same.

Clausius started to review Carnot’s other claims, specifically that “heat cannot by itself pass from a colder body to a warmer body” and Carnot’s idea about a “perfect” engine (currently called a Carnot cycle) where an object does work in 4 steps: two steps at a constant temperature, and two where no heat is absorbed or emitted.  Clausius declared that he wanted a formulation of this law that was in equation form.  While playing with the different variables, Clausius realized that the heat over the temperature

Three different men had different ideas about the heat.  Ludwig Colding experimented in Denmark, “just as it is true that the human soul is immortal, so it must also surely be a general law of nature that the forces of nature are imperishable”.  Julius von Mayer, in Germany, June 1841.

Joule didn’t know but the previous year in Germany, a chemist and medical student named Julius von Mayer had decided the same thing, “falling force and motion are equivalent to heat [and] heat must also be equivalent to motion or falling force.[16]”  However, Mayer’s understanding of basic physics was iffy and didn’t really convince much of anyone about his theory.

[1] Emilie du Chatelet to the Duke de Richelelieu (June 15, 1735) translated by Bour, I and Zinsser, J  Selected Philosophical and Scientific Writings of Emilie du Chatelet (2009) p. 16

[2] Voltaire (1737) translated and found in Hagengruber, R Emilie du Chatelet between Leibniz and Newton p. 5

[3] Emilie du Chatelet “History of Fire” translated by Bour, I and Zinsser, J  Selected Philosophical and Scientific Writings of Emilie du Chatelet (2009) p. 53

[4] Isaac Newton translation found in Smith, George, “Newton’s Philosophiae Naturalis Principia Mathematica“, The Stanford Encyclopedia of Philosophy (Winter 2008 Edition), Edward N. Zalta (ed.)

[5] Voltaire to ‘s Gravesande (February 1740) translated and found in Arianrhod, R Seduced By Logic p.?

[6] Carnot, S Motive Power of Heat (1924) p. 38

[7] Coriolis, J Du Calulation de L’effet des Machines (1829) p. 17

[8] Coriolis, J Du Calulation de L’effet des Machines (1829) p. 17

[9] Carnot, S Motive Power of Heat (English translation 1890) p. 46

[10] Carnot, S Motive Power of Heat (English translation 1890) p. 225

[11] Carnot, S Motive Power of Heat (English translation 1890) p. 225

[12] Thomson, W “On an Absolute Thermometric Scale” (1848) Mathematical and Physical Papers, Vol. 1 (1882) p. 103

[13] Thomson, W “Carnot’s theory of the motive power of heat” (1849) Mathematical and Physical Papers, Vol. 1 (1882) p. 116

[14] Thomson, W “Carnot’s theory of the motive power of heat” (1849) Mathematical and Physical Papers, Vol. 1 (1882) p. 116

[15] Thomson, W “On the Sources of Energy in Nature…” (Sept 1881)

[16] Mayer, M “On the forces of Inorganic Nature” (May 1842) translated in The London, Edinburgh and Dublin Phil. Magazine Vol. XXIV – Fourth Series (1862)p. 376

This site uses Akismet to reduce spam. Learn how your comment data is processed.