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Joseph Louis Gay-Lussac

Louis Joseph Gay-Lussac

A course in two strands: the life of the magistrate’s son from the Limousin who became the most exact experimenter of Napoleonic Paris, and the science he built, from the expansion of gases and the law of combining volumes to boron, iodine, cyanogen and the burette.

Born 6 December 1778, Saint-Léonard-de-Noblat Died 9 May 1850, Paris Combining volumes 1808 Level advanced undergraduate
Every gas expands by the same fraction per degree. Extend the measured lines (solid, 0–100 °C) and they all meet zero volume at −273 °C. Gay-Lussac’s 1802 coefficient, 1/266.67, puts the meeting point at −267 °C.
Lesson 00

How to use this course

Joseph Louis Gay-Lussac gave his name to a gas law, a law of volumes, a scale of alcoholic strength and a tower in a sulphuric acid works. Behind the names stands a single method: measure carefully, look for the simple ratio, and trust it. His law of combining volumes was the clue that led Amedeo Avogadro to molecules, and his analytical methods trained a generation of chemists, Justus von Liebig among them.

Prerequisites for Part II
  • School chemistry: balancing equations, the mole, molar mass.
  • The ideal-gas law \(pV=nRT\) and basic calculus (for Lessons 05 and 06).
  • For Lesson 06, the first law of thermodynamics in the form \(dU=\delta Q-p\,dV\).

Each technical lesson opens with a paragraph for the general reader, then states the laws precisely, derives them in modern language, and ends with exercises whose solutions are folded. Gay-Lussac worked before the modern atomic weights were settled, so the lessons point out where his data were sound and where the interpretation had to wait for others.

Reference

Timeline

1778Born 6 December at Saint-Léonard-de-Noblat in the Limousin, son of Antoine Gay, a lawyer and royal judge.
1793–94His father is imprisoned as a suspect during the Terror and released after Thermidor.
1797–98Enters the École Polytechnique at nineteen; studies with Antoine François Fourcroy, Claude-Louis Berthollet and other heirs of Antoine Lavoisier.
c. 1800Moves to the École des Ponts et Chaussées, then becomes Berthollet’s assistant at Arcueil.
1802Memoir on the expansion of gases and vapours: all gases expand equally, by about 1/267 of their volume at 0 °C per degree.
180424 August: balloon ascent with Jean-Baptiste Biot. 16 September: alone, to about 7000 m. Becomes répétiteur at Polytechnique.
1805–06With Alexander von Humboldt: the composition of air and the 2 : 1 volume ratio for water; a year of travel through Italy, Switzerland and Germany.
18068 December: elected to the physics section of the First Class of the Institut (Académie des sciences).
1807Founding member of the Société d’Arcueil. Free-expansion experiment on air.
1808With Louis Jacques Thénard, prepares potassium chemically and isolates boron. 31 December: announces the law of combining volumes.
1809Combining-volumes memoir in the Mémoires d’Arcueil. Professor of chemistry at Polytechnique (succeeding Fourcroy in 1810). First professor of physics at the new Paris Faculty of Sciences.
1810With Thénard, combustion analysis of organic substances.
1811Recherches physico-chimiques, with Thénard, in two volumes.
1813–14Memoirs on iodine, which he names iode; hydriodic and iodic acids.
1815Prepares cyanogen and analyses prussic acid; foreign member of the Royal Society.
1816Founds the Annales de chimie et de physique with François Arago.
1822President of the Académie des sciences (again in 1834).
1824Paper on indigo assay introduces the words burette and pipette. Justus von Liebig works in his laboratory.
1829Chief assayer at the Bureau de garantie of the Paris Mint.
1831Elected deputy for the Haute-Vienne; re-elected 1834 and 1837.
1832Leaves the Sorbonne for the chair of chemistry at the Muséum (Jardin des Plantes).
1839Made a peer of France by Louis-Philippe.
1843Chairman of the board of the Saint-Gobain company.
1850Dies 9 May at his residence in the Jardin des Plantes, Paris; buried in Père Lachaise.
Part I · Formation
Lesson 01

Saint-Léonard and the Revolution, 1778–1797

Joseph Louis Gay was born on 6 December 1778 in Saint-Léonard-de-Noblat, a small town on the Vienne east of Limoges. His father, Antoine Gay, was a lawyer and procurator who served as a judge at Pont-de-Noblat. To distinguish their branch from other families named Gay in the district, they added the name Lussac; father and son settled on Gay-Lussac around 1803.

He learned Latin from a local priest and then from lay teachers in the town. The Revolution reached the family directly. In late 1793, under the Law of Suspects, Antoine Gay was arrested as a former royal official and held until the fall of Robespierre in July 1794. The episode left the son with a lasting distaste for political violence and a respect for order that later shaped his politics.

At about sixteen he was sent to Paris to prepare for the new engineering schools. He studied with the abbé Dumonteil and then at private boarding schools, the last at Nanterre, where he took mathematics, English and drawing. The disruption of the period made schooling irregular, and the family’s resources were stretched. The entrance examination of the École Polytechnique, founded in 1794 and free to those who passed, was his route forward.

Lesson 02

Polytechnique and Berthollet, 1797–1802

Gay-Lussac entered the École Polytechnique at nineteen. Its chemistry teaching was the best in Europe. In his first year he heard Antoine François Fourcroy and Nicolas Vauquelin; in the second, Jean-Antoine Chaptal; in the third, Louis-Bernard Guyton de Morveau and Claude-Louis Berthollet, all of them collaborators or heirs of Antoine Lavoisier. Mathematics came from teachers in the circle of Gaspard Monge and Joseph-Louis Lagrange, and the habit of quantitative argument stayed with him.

In his third year he worked with Berthollet on bleaching linen with chlorine. Berthollet, back from Egypt with Napoleon, was looking for an assistant. Gay-Lussac passed on to the École des Ponts et Chaussées, the normal next step for a polytechnicien, but attended irregularly and was soon working full time in Berthollet’s private laboratory at Arcueil, south of Paris.

Berthollet was the most important influence on his career. He gave the young man apparatus, problems and, above all, the expectation of exact measurement. Berthollet’s neighbour at Arcueil was Pierre-Simon Laplace, whose programme of explaining heat, light and chemistry by short-range forces between particles set many of the questions Gay-Lussac would attack experimentally.

Lesson 03

Arcueil, balloons and Humboldt, 1802–1809

His first major paper, read to the Institut in 1802, showed that all gases and vapours expand by the same fraction when heated through the same range (Lesson 04). It made his reputation at 23. In 1804 the Institut, at Laplace’s urging, organized balloon ascents to test whether the Earth’s magnetism weakens with height. On 24 August Gay-Lussac and Jean-Baptiste Biot rose from the garden of the Conservatoire des Arts et Métiers to about 4000 m. On 16 September Gay-Lussac went up alone and reached about 7000 m, a height record for its time (Lesson 05). The same year he became répétiteur, an assistant teacher, at Polytechnique.

In 1805 the Prussian naturalist Alexander von Humboldt, just back from the Americas, joined him in a study of air analysis by the eudiometer. Their joint paper established that hydrogen and oxygen combine in the ratio of 2 volumes to 1, to within a fraction of a percent. The two men then travelled together for a year through France, Italy, Switzerland and Germany, measuring magnetism and air composition, visiting Vesuvius and meeting Alessandro Volta. They remained friends for life.

On 8 December 1806, aged 28, he was elected to the physics section of the First Class of the Institut. In 1807 Berthollet and Laplace formed the Société d’Arcueil, a small private academy that met at their houses and published three volumes of Mémoires; Gay-Lussac was a founding member and one of its most productive authors. In 1808 he began a long partnership with Louis Jacques Thénard, the son of a peasant from Champagne who had risen through Vauquelin’s laboratory. Their work on the alkali metals made both famous (Lesson 08). He married Geneviève Rojot, whom he had met while she was working in a Paris linen shop; they had five children.

Part II · The chemistry and physics
Lesson 04

The expansion of gases

For the general reader. Heat a gas at constant pressure and it swells. Gay-Lussac showed in 1802 that every gas swells by the same fraction for the same rise in temperature, whatever its chemical nature, and that steam above the boiling point behaves the same way. The rule is so uniform that it defines a thermometer and points to an absolute zero.

Goals
  • State the law of uniform expansion and the coefficient Gay-Lussac measured.
  • Derive absolute temperature from the linear law.
  • Understand why the law needed dry gases and careful apparatus.

The experiment

Earlier workers had found different expansions for different gases, because their gases were moist. Water vapour evaporating into a warming sample adds volume of its own. Gay-Lussac dried his gases carefully and filled a dry glass flask with a long calibrated neck, closed by a short index of mercury that moved as the gas expanded. He heated the flask in a water bath from melting ice to boiling water and read the volume change. He tested air, oxygen, hydrogen, nitrogen and several gases that dissolve readily in water, as well as the vapour of ether above its boiling point.

Law of uniform expansion (Gay-Lussac, 1802)

At constant pressure, all gases, and all vapours far enough from condensation, expand by the same fraction of their volume when heated through the same interval. Between the freezing and boiling points of water, 100 volumes become about 137.5 volumes; the expansion is uniform on the mercury scale, \(1/266.67\) of the volume at 0 °C per degree.

Gay-Lussac credited unpublished experiments made by Jacques Charles in the 1780s, which is why the law is often called Charles’s law. John Dalton reached a similar result independently in 1801, with less exact data. The modern coefficient is \(1/273.15\) per kelvin.

Absolute temperature

Write the law as \(V(\theta)=V_0(1+\alpha\theta)\), with \(\theta\) in degrees Celsius and \(\alpha\) the same for all gases. Then \(V\) vanishes at \(\theta=-1/\alpha\). Define \(T=\theta+1/\alpha\). The law becomes

\[ \frac{V}{T}=\text{constant at fixed }p, \qquad \text{or, with Boyle's law, } \qquad \frac{pV}{T}=\text{constant for a fixed amount of gas.} \]

With \(\alpha=1/266.67\) the zero lies at −266.7 °C; with the modern value it lies at −273.15 °C. Neither Gay-Lussac nor Dalton drew this conclusion. It became the basis of the absolute scale in the hands of William Thomson in 1848, by a thermodynamic argument that does not depend on any substance.

The companion law

At constant volume the same reasoning gives \(p\propto T\). Textbooks in many countries call this pressure–temperature form Gay-Lussac’s law. He did not publish it as a separate law, but it follows at once from his result combined with Robert Boyle’s law.

Exercise 4.1Using Gay-Lussac’s figure of 137.5 volumes at 100 °C for 100 volumes at 0 °C, compute \(\alpha\) and the temperature at which the extrapolated volume vanishes. Compare with the modern value.

Show solution
\(100\alpha\cdot100=37.5\), so \(\alpha=0.00375=1/266.67\) per degree. The volume vanishes at \(\theta=-1/\alpha=-266.7\) °C. The modern 136.6 volumes give \(\alpha=1/273.15\) and \(-273.15\) °C. His error of 0.9 volume in 137 came mainly from traces of moisture and the expansion of the glass.

Exercise 4.2A balloon envelope holds 600 m³ of hydrogen at 15 °C. The Sun heats the gas to 35 °C at constant pressure. How much gas must escape through the open neck, and by what fraction does the lift change? Treat the outside air as staying at 15 °C.

Show solution
\(V\propto T\): the gas would occupy \(600\times308.15/288.15=641.6\) m³, so 41.6 m³ (6.5% of the mass) escapes. Lift is (air mass displaced − gas mass) \(\times g\); displaced air is unchanged, and the hydrogen mass falls by 6.5%. Since hydrogen weighs only about 7% of the air it displaces, lift rises by about \(0.065\times0.07/0.93\approx0.5\%\).

Exercise 4.3Explain, using Dalton’s law of partial pressures, why moist air appears to expand more than dry air when heated from 0 °C to 100 °C in a flask containing a little liquid water.

Show solution
The vapour pressure of water rises from 0.6 kPa at 0 °C to 101 kPa at 100 °C. At constant total pressure, the partial pressure of air must fall as more water evaporates, so the total volume grows by much more than the expansion of the dry air alone. At 100 °C the flask would in principle fill with steam. Hence the need to dry the gas.
Lesson 05

The atmosphere at 7000 metres

For the general reader. In 1804 Gay-Lussac carried barometers, thermometers, hygrometers, magnetic needles and empty glass flasks into the sky. He wanted to know whether the Earth’s magnetism weakens with height and whether high air differs from low air. He found that magnetism changed little and that the air at 7000 metres had the same proportion of oxygen as at the ground.

Goals
  • Derive the barometric formula and use it to infer altitude from pressure.
  • Understand why constant composition with height argues for mixing.
  • Estimate the magnetic test the ascents were designed for.

Two ascents

The first ascent, with Biot on 24 August 1804, reached about 4000 m. The oscillation period of a horizontal magnetic needle was unchanged within error, contradicting a claim by Horace-Bénédict de Saussure from Alpine measurements. On 16 September Gay-Lussac went up alone with lighter instruments and more ballast. At the top his barometer stood at less than half its ground reading and the thermometer well below freezing. He opened evacuated flasks to collect air, sealed them, and analysed the samples in Paris. The oxygen fraction matched that of ground air to within the precision of his eudiometer, close to 21%.

Altitude from pressure

For an atmosphere in hydrostatic equilibrium, \(dp=-\rho g\,dz\), and for an ideal gas of molar mass \(M\), \(\rho=pM/RT\). Then

\[ \frac{dp}{p}=-\frac{Mg}{RT}\,dz \qquad\Longrightarrow\qquad z_2-z_1=\frac{R\bar T}{Mg}\,\ln\frac{p_1}{p_2}, \]

where \(\bar T\) is a suitable mean temperature of the layer (exactly the harmonic mean over height). The scale height \(H=R\bar T/(Mg)\) is about 8 km near the ground. Laplace had given a refined version of this formula, with corrections for humidity and the variation of gravity, in the Mécanique céleste; Gay-Lussac used it to reduce his barometer readings to heights.

Result (Gay-Lussac, 1804–1805)

Within experimental error, the proportion of oxygen in dry air is the same at about 7000 m as at the surface, and the horizontal intensity of the Earth’s magnetic field shows no measurable decrease over that height.

The constant composition matters. If gases were stratified by weight, each would follow its own exponential with scale height \(RT/(M_ig)\), and oxygen (\(M=32\)) would thin faster than nitrogen (\(M=28\)). Gay-Lussac’s samples showed that turbulent mixing dominates in the lower atmosphere, a conclusion consistent with Dalton’s view that each gas in a mixture acts independently but is stirred together by winds.

Exercise 5.1A barometer reads 765 mm at the ground and 329 mm at the top of an ascent. Taking a mean temperature of 9 °C for the column, \(M=0.02896\) kg/mol and \(g=9.81\) m/s², estimate the height.

Show solution
\(H=RT/(Mg)=8.314\times282/(0.02896\times9.81)=8253\) m. \(\ln(765/329)=0.844\), so \(\Delta z\approx 6960\) m, about 7 km.

Exercise 5.2Suppose oxygen and nitrogen were each in separate hydrostatic equilibrium at 250 K, with mole fractions 0.21 and 0.79 at the ground. What would the oxygen fraction be at 7000 m? Why does Gay-Lussac’s result rule this out?

Show solution
Each partial pressure falls as \(e^{-z/H_i}\), \(H_i=RT/(M_ig)\). The ratio changes by \(\exp[-gz(M_{\mathrm O_2}-M_{\mathrm N_2})/RT]=\exp[-9.81\times7000\times0.004/(8.314\times250)]=e^{-0.132}=0.876\). The oxygen fraction would be \(0.21\times0.876/(0.79+0.21\times0.876)\approx0.189\). A change from 21% to 19% was well within his detection, and he saw none: the lower atmosphere is mixed.
Lesson 06

Free expansion and the heat of gases

For the general reader. When a gas rushes into an empty vessel, does it cool? In 1807 Gay-Lussac let air flow from one globe into another and measured both. One cooled, the other warmed, and the two changes cancelled. Forty years later the same experiment, repeated by James Prescott Joule, became evidence that the energy of an ideal gas depends only on its temperature.

Goals
  • Describe the 1807 two-globe experiment.
  • Show that it implies \((\partial U/\partial V)_T=0\) for an ideal gas.
  • Connect the ratio of specific heats to Laplace’s speed of sound.

The experiment

Gay-Lussac connected two equal glass globes by a tube with a stopcock, filled one with dry air and evacuated the other. Sensitive thermometers sat inside both. When the stopcock opened, the full globe cooled and the empty one warmed by nearly the same number of degrees. He repeated the test at several initial pressures and with other gases, and always found the cooling and warming nearly equal.

His motive was the caloric theory. Many supposed that a gas’s capacity for heat depends on its volume, so that a gas allowed to expand would absorb heat. If that were so, the combined system should cool on balance. It did not. Gay-Lussac recorded the result without drawing a firm theoretical conclusion; the experiment was largely forgotten until Joule repeated it in 1845.

Joule’s law (from free expansion)

If a gas expands into a vacuum inside a rigid, insulated container with no net change of temperature, then its internal energy depends on temperature alone: \(\left(\partial U/\partial V\right)_T=0\).

Derivation. The two globes form an isolated system: no heat enters (\(Q=0\)) and the rigid walls do no work (\(W=0\)), so \(\Delta U=0\). If the final temperature equals the initial temperature while the volume has doubled, then \(U(T,2V)=U(T,V)\). The local cooling and warming arise because the gas left behind in the first globe expands and pushes the escaping gas, which is compressed in the second; work is transferred inside the system, not across its boundary.

Specific heats and sound

For an ideal gas, Joule’s law implies \(C_p-C_V=R\) per mole. The ratio \(\gamma=C_p/C_V\) governs adiabatic compression, \(pV^\gamma=\) constant. In 1816 Laplace showed that sound waves are adiabatic, so their speed is \(c=\sqrt{\gamma p/\rho}\) and not Isaac Newton’s \(\sqrt{p/\rho}\). Laplace used a measurement of \(\gamma\) made by Gay-Lussac with Jean-Joseph Welter in the early 1820s, by the sudden-expansion method of Clément and Desormes, to bring theory and the measured speed of sound into agreement.

Exercise 6.1For a van der Waals gas, \(U=C_VT-a n^2/V\). Find the temperature change when \(n\) moles expand freely from \(V\) to \(2V\) in an insulated rigid vessel. Why did Gay-Lussac see no net effect?

Show solution
\(\Delta U=0\) gives \(C_V\Delta T=an^2\left(\tfrac{1}{2V}-\tfrac1V\right)=-\tfrac{an^2}{2V}\), so \(\Delta T=-an^2/(2C_VV)\). For air at 1 atm, \(a\approx0.137\) Pa m⁶/mol², \(n/V\approx41\) mol/m³ and \(C_V/n\approx20.8\) J/(mol K), so \(\Delta T\approx-0.137\times41/(2\times20.8)\approx-0.14\) K, far below what his thermometers could resolve after heat exchange with the glass.

Exercise 6.2Air at 0 °C has density 1.293 kg/m³ at 101 325 Pa. Compute Newton’s and Laplace’s speeds of sound with \(\gamma=1.40\). The measured value is about 331 m/s.

Show solution
Newton: \(\sqrt{101325/1.293}=280\) m/s, about 15% too low. Laplace: \(\sqrt{1.40}\times280=331\) m/s, in agreement.
Lesson 07

The law of combining volumes

For the general reader. Weigh the substances in a reaction and the ratios are untidy: 8 grams of oxygen for each gram of hydrogen in water. Measure the gases by volume and the ratios become small whole numbers: exactly two volumes of hydrogen to one of oxygen. Gay-Lussac found that this simplicity holds for every reaction between gases. It was the strongest early hint that gases are made of countable particles.

Goals
  • State the law of combining volumes with Gay-Lussac’s own examples.
  • Use volume ratios and gas densities to predict the density of a compound gas.
  • See how the law leads to Avogadro’s hypothesis and why Dalton resisted it.

He announced the law to the Société philomathique on 31 December 1808 and published it in 1809 in the second volume of the Mémoires d’Arcueil. His starting point was the 2 : 1 ratio for water he had measured with Humboldt. He then noticed the same simplicity in reactions of the acid gases with ammonia, which form solid salts and so leave no gaseous product to confuse the count.

Law of combining volumes (Gay-Lussac, 1808)

Gases combine with each other in simple ratios by volume, measured at the same temperature and pressure. When the product is a gas, its volume also stands in a simple ratio to the volumes of the reacting gases, and the apparent contraction on combination is itself a simple fraction of the reacting volumes.

His examples

From his own measurements and those of others (100 volumes of the first gas in each case):

  • muriatic gas (HCl) with 100 of ammonia; carbonic gas with 200 of ammonia;
  • nitrogen with 300 of hydrogen (in ammonia);
  • nitrogen with 50, 100 and 200 of oxygen (nitrous oxide, nitrous gas and nitrogen dioxide, then called nitric acid);
  • carbonic oxide with 50 of oxygen, giving 100 of carbonic acid gas;
  • hydrogen with 50 of oxygen, giving 100 of steam.

Densities from volumes

The law lets one predict the density of a gaseous compound from those of its components. If \(a\) volumes of gas A and \(b\) of B give \(c\) volumes of product, conservation of mass gives

\[ d_{\text{product}}=\frac{a\,d_A+b\,d_B}{c}, \]

with all densities relative to air at the same temperature and pressure. Gay-Lussac used this to check the law against measured densities: for ammonia from 1 volume of nitrogen and 3 of hydrogen contracting to 2, he computed 0.594 against a measured 0.596.

Interpretation

Gay-Lussac remarked that his law fitted Dalton’s atomic theory and suggested that combining volumes might give relative numbers of atoms. Dalton disagreed. If equal volumes held equal numbers of atoms, then 1 volume of nitrogen and 1 of oxygen could make only 1 volume of nitrous gas, not the 2 observed, unless atoms split. In 1811 Avogadro resolved the paradox: equal volumes contain equal numbers of molecules, and the molecules of the elementary gases can contain two atoms. The modern equations make the volume ratios immediate:

\[ \begin{aligned} 2\,\mathrm{H_2}+\mathrm{O_2}&\to2\,\mathrm{H_2O}, & \mathrm{N_2}+3\,\mathrm{H_2}&\to2\,\mathrm{NH_3},\\ \mathrm{N_2}+\mathrm{O_2}&\to2\,\mathrm{NO}, & 2\,\mathrm{CO}+\mathrm{O_2}&\to2\,\mathrm{CO_2}. \end{aligned} \]

Exercise 7.1Densities relative to air are: hydrogen 0.0696, nitrogen 0.967. Use 1 volume nitrogen + 3 volumes hydrogen → 2 volumes ammonia to compute the density of ammonia, and compare with Gay-Lussac’s figures.

Show solution
\(d=(0.967+3\times0.0696)/2=1.176/2=0.588\). Gay-Lussac, with the densities of his day, obtained 0.594; the modern value is 0.597 at 0 °C. Ammonia deviates slightly from ideal behaviour, which accounts for part of the gap.

Exercise 7.2Gay-Lussac reported that 100 volumes of carbonic oxide combine with 50 of oxygen to give 100 of carbonic acid gas. Show that the contraction equals the volume of oxygen used, and explain this in terms of molecules.

Show solution
Reactants 150 volumes, product 100: contraction 50, equal to the oxygen. In \(2\,\mathrm{CO}+\mathrm{O_2}\to2\,\mathrm{CO_2}\) three molecules become two, and the lost molecule corresponds to the oxygen added; each O\(_2\) is split between two CO molecules.

Exercise 7.3Gaseous hydrogen chloride and ammonia combine in equal volumes to form a white solid. What does Avogadro’s hypothesis say about the formula of the solid, and why are such reactions useful for testing the law?

Show solution
Equal volumes mean equal numbers of molecules, so the solid contains HCl and NH\(_3\) in a 1 : 1 ratio, NH\(_4\)Cl. Because the product is a solid, no gas remains at the end except any excess reactant, whose volume is read directly. The ratio is measured without needing the density or volume of a gaseous product.
Lesson 08

Potassium, boron, chlorine and iodine

For the general reader. In 1807 Humphry Davy used a giant battery to tear potassium out of potash. Napoleon’s savants answered with chemistry. Gay-Lussac and Thénard made potassium by heating potash with iron, in quantities large enough to use as a reagent, and with it they isolated boron. Over the next six years Gay-Lussac also helped show that chlorine and iodine are elements, and that acids need not contain oxygen.

Goals
  • Write the reactions by which Gay-Lussac and Thénard made potassium and boron.
  • Understand the debate over “oxymuriatic acid” and the concept of hydracids.
  • Follow the identification of iodine as an element.

Potassium and boron (1808)

Davy’s electrolysis yielded tiny amounts of metal. Gay-Lussac and Thénard passed molten potash over red-hot iron filings in a gun barrel and collected potassium by the gram. An explosion in this work seriously injured Gay-Lussac’s eyes. They then heated boric acid with potassium in a copper tube and obtained an olive-brown powder, a new element they called bore. They announced it in 1808, at nearly the same time as Davy, who isolated boron by a similar route that year.

\[ \mathrm{B_2O_3}+6\,\mathrm{K}\longrightarrow2\,\mathrm B+3\,\mathrm{K_2O}. \]

For this work the pair received the prize Napoleon had founded for advances in galvanism, in 1809. Their two-volume Recherches physico-chimiques (1811) collected these and many other experiments.

Chlorine and the hydracids

Following Lavoisier, chemists held that every acid contains oxygen. Chlorine was therefore “oxygenated muriatic acid”, an oxide of an unknown radical. In 1809 Gay-Lussac and Thénard found that no means could extract oxygen from it; even charcoal heated in it gave no carbonic acid. They noted that it could be treated as an element but did not insist. Davy argued firmly in 1810 that it is an element and named it chlorine. Muriatic acid is then simply HCl, an acid with no oxygen.

Iodine (1813–1814)

In 1811 the saltpetre maker Bernard Courtois noticed violet vapour rising from seaweed ash treated with sulphuric acid. Samples went to several chemists. Gay-Lussac and Davy, who was visiting Paris in 1813 with special permission despite the war, worked on it at the same time. Gay-Lussac named it iode, from the Greek for violet, and in his memoir of 1814 described it as an element analogous to chlorine. He prepared hydriodic acid HI and iodic acid, and concluded that acidity does not require oxygen. He introduced the term hydracide for acids of hydrogen with a non-metal, extending the class later to hydrofluoric acid.

Analogy (Gay-Lussac, 1814)

Chlorine and iodine form parallel series: HCl and HI are both strong acids formed from equal volumes of hydrogen and halogen vapour, giving two volumes of acid gas; both elements form oxyacids and combine with metals in the same proportions.

Exercise 8.1How much potassium is needed to reduce 10 g of boron trioxide, and how much boron results? (B = 10.81, O = 16.00, K = 39.10.)

Show solution
\(M(\mathrm{B_2O_3})=69.62\), so 10 g is 0.1436 mol. Potassium needed: \(6\times0.1436=0.862\) mol, 33.7 g. Boron produced: \(2\times0.1436\times10.81=3.10\) g. Each gram of boron costs about 11 g of potassium.

Exercise 8.2The density of iodine vapour relative to air is about 8.7 and that of hydrogen 0.0696. Using equal volumes of hydrogen and iodine vapour giving two volumes of HI, predict the density of hydrogen iodide relative to air. (Measured: about 4.4.)

Show solution
\(d=(0.0696+8.7)/2=4.38\). Agreement supports both the volume law and the formula HI with diatomic H\(_2\) and I\(_2\).
Lesson 09

Cyanogen, radicals and organic analysis

For the general reader. Plants and animals are made of a few elements: carbon, hydrogen, oxygen and nitrogen. To find their proportions you must burn the substance completely and weigh or measure what comes out. Gay-Lussac and Thénard built the first reliable method in 1810. In 1815 Gay-Lussac found that a group of atoms, carbon with nitrogen, can pass unchanged through reactions like a single element. He had discovered the first compound radical.

Goals
  • Calculate an empirical formula from combustion data.
  • Understand the cyanogen radical and its analogy with the halogens.
  • Write Gay-Lussac’s equation for alcoholic fermentation.

Combustion analysis (1810)

Gay-Lussac and Thénard mixed a weighed organic sample with potassium chlorate, pressed it into pellets, and dropped them one by one into a heated vertical tube. The gases were collected over mercury. They measured the oxygen consumed and the carbonic acid formed, and inferred hydrogen from the balance. Later Gay-Lussac replaced chlorate with copper oxide, which is safer. Liebig, who learned the method in Paris, turned it into the standard five-bulb apparatus of the 1830s.

From their analyses Gay-Lussac also gave the overall equation of alcoholic fermentation, in modern form

\[ \mathrm{C_6H_{12}O_6}\longrightarrow2\,\mathrm{C_2H_5OH}+2\,\mathrm{CO_2}. \]

Prussic acid and cyanogen (1815)

Carl Wilhelm Scheele had made prussic acid (HCN) from Prussian blue in 1782. Gay-Lussac prepared the pure anhydrous acid and showed that it contains no oxygen. Heating mercuric cyanide, he obtained a colourless, poisonous gas that burns with a peach-coloured flame. He analysed it by combustion: 1 volume gave 2 volumes of carbonic acid and 1 volume of nitrogen, so its formula is C\(_2\)N\(_2\). He named it cyanogène, generator of blue.

\[ \mathrm{Hg(CN)_2}\xrightarrow{\ \text{heat}\ }\mathrm{Hg}+\mathrm{(CN)_2}. \]
Cyanogen as a radical (Gay-Lussac, 1815)

The group CN passes unchanged through a series of compounds and behaves like a halogen atom: (CN)\(_2\) parallels Cl\(_2\), HCN parallels HCl, and KCN parallels KCl. A compound body can therefore play the role of an element in chemical combination.

This was the first clear example of a compound radical. Liebig and Friedrich Wöhler’s benzoyl radical (1832) and the radical theory of organic chemistry built on it. In 1824 Liebig, working in Gay-Lussac’s laboratory, analysed silver fulminate; Wöhler at the same time analysed silver cyanate. The two salts had the same composition and different properties, an early case of isomerism, which Jöns Jacob Berzelius named in 1830.

Exercise 9.1Combustion of 0.230 g of a compound containing only C, H and O gives 0.440 g CO\(_2\) and 0.270 g H\(_2\)O. Find its empirical formula. Its vapour density relative to hydrogen gas is 23; find the molecular formula.

Show solution
C: \(0.440\times12/44=0.120\) g (0.0100 mol). H: \(0.270\times2/18=0.0300\) g (0.0300 mol). O: \(0.230-0.150=0.080\) g (0.0050 mol). Ratio C : H : O = 2 : 6 : 1, so C\(_2\)H\(_6\)O. Molar mass \(2\times23=46\), equal to the empirical formula mass: ethanol (or dimethyl ether).

Exercise 9.2Write the combustion of cyanogen and show that 1 volume gives 2 volumes of CO\(_2\) and 1 of N\(_2\). How many volumes of oxygen are consumed?

Show solution
\(\mathrm{C_2N_2}+2\,\mathrm{O_2}\to2\,\mathrm{CO_2}+\mathrm N_2\). By Avogadro, volumes are in the ratio of molecules: 1 of cyanogen and 2 of oxygen give 2 of CO\(_2\) and 1 of nitrogen. Gay-Lussac used exactly these ratios to fix the formula.
Lesson 10

Volumetric analysis and industrial chemistry

For the general reader. To find how much silver is in a coin, you can dissolve it and add salt water drop by drop until no more silver chloride forms. The volume of salt solution used tells you the silver. Gay-Lussac turned this idea into a precise method for the Paris Mint and gave chemistry the burette and the pipette. He also measured the strength of spirits for the tax office and cut the pollution of sulphuric acid works.

Goals
  • Do a titration calculation in the style of Gay-Lussac’s silver assay.
  • Understand the principle of the alcoholometer.
  • See how the Gay-Lussac tower recovers nitrogen oxides in the lead-chamber process.

Burette and pipette

Titration was older; François-Antoine Descroizilles had used a graduated tube in the 1790s to test bleach. Gay-Lussac made it exact. In his 1824 paper on standardizing indigo solutions for bleach assay he introduced the words burette and pipette, and described an improved burette with a side arm.

The silver assay

As assayer to the Mint from 1829, Gay-Lussac replaced the old fire assay (cupellation), which lost silver and gave errors of several parts per thousand, by a wet method published in 1832. A sample is dissolved in nitric acid and titrated with a standard sodium chloride solution:

\[ \mathrm{Ag^+}+\mathrm{Cl^-}\longrightarrow\mathrm{AgCl}\downarrow. \]

Near the end point he added the salt in small decimal portions, shaking until the precipitate settled and the liquid cleared, and watched whether a further drop still gave a cloud. The method was far more precise than cupellation and was adopted by mints across Europe.

Alcoholometry

In 1824 a French law based the tax on spirits on his measurements. Gay-Lussac determined the densities of water–ethanol mixtures as a function of composition and temperature and built a hydrometer graduated directly in percentage of alcohol by volume at 15 °C. The “degree Gay-Lussac” (°GL) is still used for the strength of wines and spirits.

The Gay-Lussac tower

In the lead-chamber process for sulphuric acid, nitrogen oxides catalyse the oxidation of sulphur dioxide and then escape with the exhaust. Gay-Lussac proposed in 1827 to absorb them in a tower packed with coke, down which concentrated sulphuric acid trickles, forming nitrosylsulphuric acid. John Glover’s tower (1859) later released the oxides at the front of the plant. The Gay-Lussac tower was first installed at the Chauny works of the Saint-Gobain company, which Gay-Lussac served as director and, from 1843, as chairman.

Exercise 10.1A 1.000 g sample of coin alloy is dissolved in nitric acid. It requires 83.10 mL of 0.1000 mol/L NaCl to reach the end point. Find the fineness in parts per thousand (Ag = 107.87).

Show solution
Moles of Cl\(^-\) = \(0.08310\times0.1000=8.310\times10^{-3}\), equal to moles of Ag. Mass of Ag = \(8.310\times10^{-3}\times107.87=0.8964\) g. Fineness 896 per thousand, close to the 900 of French silver coin.

Exercise 10.2An assayer wants to dispense a fixed volume of salt solution that precipitates exactly 1 g of silver. What concentration of NaCl, in grams per litre, gives this in a 100 mL pipette? (Na = 22.99, Cl = 35.45.)

Show solution
1 g Ag is \(1/107.87=9.270\times10^{-3}\) mol, needing the same amount of NaCl, \(9.270\times10^{-3}\times58.44=0.5418\) g in 100 mL. Concentration 5.418 g/L. Gay-Lussac’s normal solution was designed on exactly this principle, so that one pipette corresponds to one gram of silver.

Exercise 10.3A mixture is 40% ethanol by volume at 15 °C. Why can it not be prepared by mixing 40 mL of ethanol with 60 mL of water, and why must an alcoholometer be calibrated empirically?

Show solution
Ethanol and water contract on mixing (by up to about 4% near 50–60% ethanol), so 40 + 60 mL gives less than 100 mL and the result is above 40% by volume. Because the contraction and the density both depend on composition and temperature in a way no simple rule predicts, Gay-Lussac had to tabulate densities by experiment and calibrate the hydrometer from those tables.
Part III · Life and legacy
Lesson 11

Professor, editor, deputy, 1809–1840

From 1809 Gay-Lussac held a chair of chemistry at the École Polytechnique, becoming its chief chemistry professor after Fourcroy’s death in 1810, and the first chair of physics at the new Faculty of Sciences of Paris. He held the Sorbonne chair until 1832, when he moved to the chair of chemistry at the Muséum d’histoire naturelle, and left Polytechnique in 1840, succeeded by his former assistant Théophile-Jules Pelouze. Students remembered a clear, careful lecturer who described his own discoveries with conspicuous modesty.

His laboratory drew foreign students. Justus von Liebig arrived in Paris in 1822, was introduced by Humboldt, and in 1824 worked with Gay-Lussac on the fulminates. Liebig later described those months as decisive, and modelled his famous teaching laboratory at Giessen partly on what he had seen. Gay-Lussac’s eldest son Jules later studied under Liebig at Giessen.

In 1816 he and François Arago, his closest friend, took over the Annales de chimie as the Annales de chimie et de physique, which they edited for decades and which became one of the leading journals of physical science. He was president of the Académie des sciences in 1822 and 1834. He served on government committees for gunpowder and saltpetre, for arts and manufactures, and as assayer to the Mint, posts that brought both income and influence over French industry.

After the July Revolution he entered politics. He was elected deputy for the Haute-Vienne in 1831 and re-elected in 1834 and 1837, sitting with the moderate supporters of the July Monarchy, while Arago sat on the left. In 1839 Louis-Philippe made him a peer of France. In the Chamber of Peers he spoke on industrial and technical questions; he opposed a bill to limit child labour in factories, and lost.

DiscussionGay-Lussac combined academic research with paid service to the state and to industry, on the Mint, the spirits tax and the Saint-Gobain board. What did each side gain from this arrangement, and what conflicts of interest could it create?

Lesson 12

Last years, death and legacy, 1840–1850

In his last decade Gay-Lussac gave more time to Saint-Gobain and to his duties at the Mint, while still experimenting; an explosion during work on hydrocarbon gases in 1844 injured him again. The Revolution of 1848 ended the Chamber of Peers, and he resigned his post at the Mint, which passed to his son Jules. He died after a short illness on 9 May 1850 at his residence in the Jardin des Plantes, aged 71, and was buried in the Père Lachaise cemetery.

Legacy

  • Gas laws: the uniform expansion of gases is a foundation of the ideal-gas law and of absolute temperature; in many countries the pressure–temperature law carries his name.
  • Atoms and molecules: the law of combining volumes led directly to Avogadro’s hypothesis (1811) and, through Stanislao Cannizzaro in 1858–60, to consistent atomic weights.
  • Elements and radicals: boron, the elementary status of chlorine and iodine, the idea of oxygen-free acids, and the cyanogen radical.
  • Analytical chemistry: combustion analysis, volumetric titration with burette and pipette, the silver assay and alcoholometry.
  • Honours: foreign member of the Royal Society (1815) and of the Royal Swedish Academy of Sciences (1821); grand officer of the Legion of Honour; the Prussian Pour le Mérite (1842). His name is among the 72 engraved on the Eiffel Tower, and a lunar crater bears it.

Final projectChoose one of Gay-Lussac’s quantitative results: the expansion coefficient of 1802, the combining volumes of 1808, or the composition of cyanogen. Reproduce the numbers from modern data, estimate the experimental error he would have faced, and explain what he could and could not conclude from it in his own time.

Reference

Sources and further reading

Biography

  1. M. Crosland, Gay-Lussac: Scientist and Bourgeois, Cambridge University Press, 1978. The standard biography.
  2. M. Crosland, The Society of Arcueil: A View of French Science at the Time of Napoleon I, Heinemann, 1967.
  3. Joseph Louis Gay-Lussac, Wikipedia; Louis Joseph Gay-Lussac, Wikipédia (French).
  4. P. Jolibois, Notice on Gay-Lussac, Académie des sciences, 1950.
  5. Gay-Lussac, Louis Joseph, Encyclopædia Universalis.

Science

  1. J. L. Gay-Lussac, Recherches sur la dilatation des gaz et des vapeurs, Annales de chimie 43 (1802), 137–175.
  2. J. L. Gay-Lussac and A. von Humboldt, Expériences sur les moyens eudiométriques et sur la proportion des principes constituants de l’atmosphère, Journal de physique 60 (1805).
  3. J. L. Gay-Lussac, Memoir on the combination of gaseous substances with each other, Mémoires de la Société d’Arcueil 2 (1809), 207; English translation in the Classic Chemistry collection, Le Moyne College.
  4. J. L. Gay-Lussac and L. J. Thénard, Recherches physico-chimiques, 2 vols., Paris, 1811.
  5. J. L. Gay-Lussac, Mémoire sur l’iode, Annales de chimie 91 (1814).
  6. J. L. Gay-Lussac, Recherches sur l’acide prussique, Annales de chimie 95 (1815).
  7. J. L. Gay-Lussac, Instruction sur l’essai des matières d’argent par la voie humide, Paris, 1832.
  8. A. J. Ihde, The Development of Modern Chemistry, Harper & Row, 1964; Dover reprint 1984.