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Robert Boyle

The Honourable Robert Boyle FRS

A course in two strands: the life of the Irish earl’s son who made the laboratory a place of public, repeatable experiment, and the physics and chemistry of air, pressure, elements, fire and corpuscles that he measured and argued about.

Born 25 January 1627, Lismore Castle, County Waterford Died 31 December 1691, London Boyle’s law 1662 Level advanced undergraduate
Boyle’s table of the condensation of the air (1662). Dots: measured pressure in inches of mercury against the length of the trapped air column. Curve: the hypothesis that pressure and volume are reciprocal, \(pV=\text{const}\).
Lesson 00

How to use this course

Robert Boyle is remembered in every physics course for one law, and in every chemistry course as a founder of the subject. Neither memory captures him well. His great contribution was a method: careful experiments with instruments, reported in enough detail that others could repeat them, and witnessed by a community of gentlemen who judged the results. The air pump, built for him by Robert Hooke, was its showpiece. The law of pressure and volume was one result among hundreds.

Prerequisites for Part II
  • First-year mechanics: pressure, density, hydrostatic equilibrium.
  • Basic thermodynamics: the ideal gas law \(pV=nRT\) and the mole.
  • Introductory chemistry: balanced equations, molar masses, acids and bases.
  • For Lesson 08, the kinetic description of a gas; for Lesson 10, the van der Waals equation is helpful but is developed in the lesson.

Each technical lesson opens with a paragraph for the general reader, then gives precise statements, derivations and exercises with folded solutions. Where a lesson uses modern ideas that Boyle did not have (moles, molecules, the van der Waals equation), it says so. Dates before 1752 are in the Old Style (Julian) calendar used in England at the time.

Reference

Timeline

1627Born 25 January at Lismore Castle, County Waterford, seventh son and fourteenth child of Richard Boyle, 1st Earl of Cork, and Catherine Fenton.
c. 1635–38At Eton College with his brother Francis.
1639–44Continental education with a French tutor: Geneva, then Italy. In Florence in the winter of 1641–42, when Galileo dies at nearby Arcetri.
1643His father dies. Robert inherits the manor of Stalbridge in Dorset and lands in Ireland.
1644Returns to England in the summer.
1646Settled at Stalbridge; writes of the “invisible college” of experimental philosophers. Sets up a laboratory.
1652–53In Ireland managing his estates.
c. 1654–56Settles in Oxford among John Wilkins’s experimental club. Engages Robert Hooke as assistant.
1659The air pump (“pneumatical engine”) is completed.
1660New Experiments Physico-Mechanicall, Touching the Spring of the Air. 28 November: present at the meeting that founds the Royal Society.
1661The Sceptical Chymist and Certain Physiological Essays.
1662Second edition of New Experiments, with A Defence of the Doctrine touching the Spring and Weight of the Air: the law \(pV=\text{const}\).
1663Named to the council of the Royal Society in its second charter. Usefulness of Experimental Natural Philosophy.
1664–66Experiments and Considerations Touching Colours (1664), History of Cold (1665), Hydrostatical Paradoxes and The Origin of Forms and Qualities (1666).
1668Moves to London, to the house of his sister Katherine, Lady Ranelagh, in Pall Mall.
1669A Continuation of New Experiments.
1670June: a stroke leaves him paralysed for a time; he recovers slowly.
1680Elected President of the Royal Society; declines because of a scruple about the oaths. Publishes his preparation of phosphorus.
1686–90A Free Enquiry into the Vulgarly Received Notion of Nature (1686), Disquisition about the Final Causes of Natural Things (1688), The Christian Virtuoso and Medicina Hydrostatica (1690).
1691His sister Katherine dies; a week later, on 31 December, Boyle dies in Pall Mall. Buried at St Martin-in-the-Fields.
1692First Boyle Lectures, endowed in his will, given by Richard Bentley. The General History of the Air appears posthumously.
Part I · Formation
Lesson 01

Lismore, Eton and the Grand Tour, 1627–1644

Robert Boyle was born on 25 January 1627 at Lismore Castle in County Waterford, Ireland. His father, Richard Boyle, had arrived in Ireland as an almost penniless adventurer and became, through land deals in Munster, one of the richest men in the British Isles and the 1st Earl of Cork. Robert was his seventh son and fourteenth child, by his second wife, Catherine Fenton. Twelve of the fifteen children survived childhood. Robert’s mother died when he was small, and the boy was sent out to nurse in the Irish countryside, a practice his father favoured for toughening children.

Around 1635 Robert and his brother Francis were sent to Eton College, whose provost was the diplomat and poet Sir Henry Wotton. He was a bookish boy, and the earl withdrew both sons in 1638. In 1639 the two brothers set out for the Continent with a French tutor. They studied in Geneva, where Robert learned French, Latin, rhetoric, religion and some mathematics. In Geneva, during a violent thunderstorm, he had a religious experience that he later described as a conversion, and his piety shaped the rest of his life.

Florence, 1641–42

In 1641 the brothers travelled into Italy. Robert learned Italian and spent the winter of 1641–42 in Florence. There he read the works of Galileo Galilei, who was living under house arrest at Arcetri, just outside the city, and who died there in January 1642. Boyle later recalled that this encounter with Galileo’s “paradoxes” turned him toward natural philosophy. The family’s fortunes, meanwhile, collapsed with the Irish rebellion of 1641. Money stopped arriving, and the young men were stranded for a time in Marseilles. Robert returned to England in the summer of 1644, in the middle of the Civil War. His father had died in September 1643.

Lesson 02

Stalbridge and the Invisible College, 1644–1654

From his father Boyle inherited the manor of Stalbridge in Dorset and estates in Ireland. He lived first with his sister Katherine, Lady Ranelagh, in London. She was thirteen years older, a woman of wide learning and strong Protestant and reforming views, and she remained the closest person in his life. By 1646 he had settled at Stalbridge, where he stayed for about six years.

At Stalbridge he wrote moral and devotional essays and, increasingly, worked with his hands. He had a furnace built and set up a chemical laboratory. Through his sister he joined the circle of reformers around Samuel Hartlib, who promoted useful knowledge, agriculture, medicine and education. In letters of 1646 and 1647 Boyle mentioned an “invisible college” of people who cared about practical learning. Historians still debate exactly whom he meant, but the phrase became attached to the groups that later formed the Royal Society. He read Pierre Gassendi, Marin Mersenne and William Oughtred, admired Copernican astronomy, and began to think of matter as made of small particles in motion.

In 1652 he went to Ireland to secure his estates. Cromwell’s land settlement left him very rich, with an independent income for life. He disliked Ireland, but he used his time there to learn anatomy by dissection with William Petty. In 1653 he met John Wilkins in London, and Wilkins urged him to come to Oxford.

Lesson 03

Oxford, Hooke and the air pump, 1654–1668

Boyle settled in Oxford in the mid-1650s, renting rooms at Cross Hall. He never held a university post. Oxford under the Commonwealth had an extraordinary concentration of experimental talent around Wilkins, Warden of Wadham College: the mathematicians John Wallis and Seth Ward, the young Christopher Wren, the physicians Thomas Willis and Richard Lower, and William Petty. Boyle’s private laboratory became one of the centres of this club.

To run his experiments he hired assistants. The most important was Robert Hooke, who had come to Oxford as a poor chorister and worked for Willis. In 1657 Boyle read of Otto von Guericke’s experiments in Magdeburg with an evacuated vessel. Guericke’s pump had to be worked under water and was hard to use. Boyle asked Hooke to design a better one. The “pneumatical engine” was finished in 1659: a glass receiver on top of a brass cylinder, with a piston worked by a rack and pinion, and a stopcock and valve to let air out stroke by stroke.

The book that came out of it, New Experiments Physico-Mechanicall, Touching the Spring of the Air and its Effects (1660), reported forty-three experiments in the form of letters to his nephew. It was written so that readers could follow, judge and repeat every step. Two critics replied. The Jesuit Franciscus Linus denied that air could exert such force and proposed an invisible membrane, the funiculus, that pulled the mercury up. Thomas Hobbes denied that experiments with a leaky machine could settle anything about the vacuum. Boyle’s answer to Linus in 1662 contained the law of Lesson 05. The quarrel with Hobbes was about what counts as knowledge, and it is the subject of a celebrated study by Steven Shapin and Simon Schaffer.

On 28 November 1660, after a lecture by Wren at Gresham College, twelve men including Boyle, Wilkins and Wren agreed to found a society for promoting physico-mathematical experimental learning. It became the Royal Society, chartered in 1662 and again in 1663, when Boyle was named to its council. In November 1662, on Boyle’s recommendation, Hooke became its Curator of Experiments. In 1668 Boyle left Oxford for London.

Part II · The physics and chemistry
Lesson 04

The pneumatical engine

For the general reader. Evangelista Torricelli had shown in 1644 that the atmosphere holds up a column of mercury about 76 cm tall. Boyle wanted to know what happens when the air is taken away. With Hooke’s pump he put candles, bells, barometers, animals and bladders inside a glass globe and pumped it out. Flames went out, sound faded, mercury fell and animals died. Air, it turned out, was a material with weight and springiness, and it was needed for fire and life.

Goals
  • Model the pump stroke by stroke and compute how fast the pressure falls.
  • Understand the “experiment in the experiment”: a barometer inside the receiver.
  • Distinguish the weight of the air from its spring.

Stroke by stroke

Let the receiver have volume \(V\) and the cylinder swept volume \(v\). At the start of a stroke the receiver holds air at pressure \(p_k\). The valve between them opens and the piston is drawn down, so the same air fills \(V+v\). Then the valve closes and the cylinder is emptied to the atmosphere. If the temperature does not change, Boyle’s law (Lesson 05) gives

Proposition (ideal pump)

After \(k\) strokes, \(\displaystyle p_k = p_0\Big(\frac{V}{V+v}\Big)^{k}\). The pressure falls geometrically and reaches zero only in the limit \(k\to\infty\).

A real pump also has a dead volume \(d\) between valve and piston, which still holds air at atmospheric pressure \(p_0\) when the piston returns. Mixing that air with the receiver’s gives the recurrence \(p_{k+1}=(p_kV+p_0d)/(V+v+d)\). Its fixed point satisfies \(p_\ast(v+d)=p_0d\), so \(p_\ast=p_0\,d/(v+d)\approx p_0\,d/v\). Leaks around the piston and stopcock set a similar floor. Hobbes made the most of these imperfections.

The barometer in the receiver

In one of the most famous experiments of the 1660 book, Boyle placed a Torricellian tube with its dish of mercury inside the receiver and sealed it in. As he pumped, the mercury column sank; when he let air back in, it rose again. The height of the column measures the pressure of the air on the dish:

\[ p = \rho_{\mathrm{Hg}}\,g\,h, \qquad \rho_{\mathrm{Hg}}=13\,595\ \mathrm{kg\,m^{-3}}. \]

This settled for Boyle that the column is held up by the air outside, against those who said nature abhors a vacuum. He never got the column all the way down, which he attributed to the pump’s leaks.

Weight versus spring

Inside a sealed receiver there is no tall column of air above the dish, yet the barometer stands at full height until the pumping begins. So it cannot simply be the weight of the air in the receiver that supports the mercury. Boyle’s explanation was that the enclosed air keeps the pressure it had when sealed, because air acts like a compressed spring. In the open atmosphere the spring of the lower air is wound up by the weight of all the air above it. The two descriptions agree in equilibrium: pressure is the spring of the local air, and it equals the weight of the column above per unit area.

Exercise 4.1A receiver of volume 8 litres is served by a cylinder of swept volume 1 litre. How many strokes reduce the pressure below 1% of atmospheric, ignoring leaks and dead volume? With a dead volume of 10 cm³, what is the lowest pressure attainable?

Show solution
We need \((8/9)^k<0.01\), so \(k>\ln 100/\ln(9/8)=4.605/0.1178=39.1\): 40 strokes. With dead volume, the fixed point is \(p_\ast=p_0d/(v+d)=p_0\cdot10/1010\approx0.0099\,p_0\). The dead volume alone stops the pump at about 1% of an atmosphere, roughly 7.6 mm of mercury.

Exercise 4.2A barometer inside the receiver reads 76.0 cm before pumping. After a number of strokes it reads 19.0 cm. A small, limp, sealed bladder in the receiver had volume 50 cm³ at the start. Estimate its volume now, assuming the bladder’s skin exerts no force.

Show solution
The pressure has fallen by a factor 4, so by Boyle’s law the bladder’s air expands by a factor 4, to about 200 cm³. Boyle reported exactly this kind of swelling: a nearly empty lamb’s bladder puffed up and even burst as the receiver was exhausted.
Lesson 05

The spring of the air: Boyle’s law

For the general reader. Squeeze a sealed bicycle pump and it pushes back harder the more you squeeze. Boyle measured how much harder. Halve the volume of a fixed amount of air and its pressure doubles; reduce the volume to a third and the pressure triples. He published this in 1662, to answer a critic who doubted that air could push so strongly.

Goals
  • Reconstruct the J-tube experiment and reduce Boyle’s own table to \(pV=\text{const}\).
  • Estimate the scatter of his data.
  • Derive two modern consequences: isothermal compressibility and isothermal work.

The J-tube

Boyle and his assistants took a long glass tube bent into a J, with the short arm sealed. Mercury poured into the open long arm trapped air in the short arm. At first the levels were equal, so the trapped air was at atmospheric pressure, measured as \(29\tfrac18\) inches of mercury. As more mercury was added, the trapped column shortened. Because the short arm had uniform bore, the volume of the air was proportional to its length, measured in “spaces” of a quarter of an inch, starting from 48.

Boyle’s law (1662)

For a fixed quantity of air at constant temperature, the pressure \(p\) and volume \(V\) satisfy \(pV=\text{constant}\). In Boyle’s apparatus the pressure on the trapped air is \(p=p_{\mathrm{atm}}+\rho g\,\Delta h\), where \(\Delta h\) is the difference of the mercury levels in the two arms.

Boyle’s table gave, for each length \(A\) of the air column, the mercury difference, the atmosphere’s \(29\tfrac18\) inches, their sum \(D\) (the total pressure), and a final column of what “that pressure should be according to the hypothesis” that pressures and volumes are reciprocal. A selection:

Length \(A\) (¼ in)Measured pressure \(D\) (in Hg) · Hypothesis \(48\times29\tfrac18/A\) · Product \(A\cdot D\)
48\(29\tfrac{2}{16}\) · \(29\tfrac{2}{16}\) · 1398
40\(35\tfrac{5}{16}\) · \(35\) · 1412.5
32\(44\tfrac{3}{16}\) · \(43\tfrac{11}{16}\) · 1414
24\(58\tfrac{13}{16}\) · \(58\tfrac{2}{8}\) · 1411.5
16\(87\tfrac{14}{16}\) · \(87\tfrac{3}{8}\) · 1406
12\(117\tfrac{9}{16}\) · \(116\tfrac{4}{8}\) · 1410.75

Across all 25 rows the product \(A\cdot D\) lies between about 1396 and 1415, a spread of roughly ±0.7% about its mean, while the pressure itself varies by a factor of four. Boyle published a second table for rarefaction, in which air trapped at the top of a tube dipped in a deep cistern of mercury was expanded by raising the tube. It showed the same law at pressures below one atmosphere.

Who found it

Boyle credited the hypothesis to Richard Towneley, who had read an account of experiments made by Henry Power in Yorkshire and Lancashire. Hooke built and probably operated the apparatus. Edme Mariotte found the same relation independently in France in the 1670s and added the observation that air expands when heated, so in France the law often carries his name. What Boyle contributed was the decisive published test, against a theory (Linus’s funiculus) that predicted something else.

Modern consequences

Combined with the later laws of Charles and Gay-Lussac and with Avogadro’s hypothesis, Boyle’s law becomes the ideal gas law \(pV=nRT\). Two consequences at fixed \(T\):

\[ \kappa_T = -\frac1V\Big(\frac{\partial V}{\partial p}\Big)_T = \frac1p, \qquad W_{1\to2} = -\int_{V_1}^{V_2} p\,dV = nRT\ln\frac{V_1}{V_2}. \]

The first says that air becomes stiffer exactly in proportion to how hard it is already squeezed. The second is the work done on the gas in an isothermal compression.

Exercise 5.1Check one row of Boyle’s table. At \(A=24\) he recorded a mercury difference of \(29\tfrac{11}{16}\) inches. Compute the total pressure, the hypothesis value and the percentage discrepancy.

Show solution
Total: \(29\tfrac{11}{16}+29\tfrac{2}{16}=58\tfrac{13}{16}=58.8125\) in. Hypothesis: \(48\times29.125/24=58.25\) in. Discrepancy \(0.5625/58.25\approx0.97\%\). The measured pressure is slightly high, as it is in most rows; small temperature changes, the meniscus and the difficulty of reading the long column are all candidates.

Exercise 5.2Show that if pressure and volume are reciprocal, the points \((\ln A,\ln D)\) lie on a line of slope \(-1\). Using the end rows \((48, 29.125)\) and \((12, 117.5625)\), estimate the slope from Boyle’s data.

Show solution
\(DA=c\) gives \(\ln D=\ln c-\ln A\), slope \(-1\). From the data, slope \(=\dfrac{\ln117.5625-\ln29.125}{\ln12-\ln48}=\dfrac{1.3954}{-1.3863}\approx-1.0066\). The exponent is \(-1\) to within 0.7%.

Exercise 5.3One mole of air at 288 K is compressed isothermally from 48 to 12 units of volume, as in Boyle’s table. How much work is done on it, and where does the energy go?

Show solution
\(W=RT\ln 4=8.314\times288\times1.386\approx3.32\ \mathrm{kJ}\). For an ideal gas at constant temperature the internal energy is unchanged, so the same 3.32 kJ leaves as heat to the glass and mercury. Done quickly, the compression would warm the air and the pressure would rise above Boyle’s values.
Lesson 06

Hydrostatical paradoxes and specific gravity

For the general reader. Water in a narrow tube can balance a much larger mass of water in a wide vessel, as long as the surfaces stand at the same height. This looked paradoxical in the seventeenth century. In Hydrostatical Paradoxes (1666) Boyle demonstrated such effects with real apparatus. At the end of his life, in Medicina Hydrostatica (1690), he turned the same principles into a practical test for detecting fake gems, debased coins and adulterated drugs: weigh them in air and in water.

Goals
  • Derive the hydrostatic law \(p=p_0+\rho gh\) and the hydrostatic paradox.
  • Compute specific gravity by double weighing.
  • Find the composition of a two-metal alloy from its specific gravity.

Pressure depends only on depth

Consider a small vertical prism of fluid of cross-section \(dA\) and height \(dz\) at rest. Balance of forces gives \(dp/dz=-\rho g\). For an incompressible fluid,

Hydrostatic law

In a connected body of fluid of constant density \(\rho\) at rest under gravity, \(p(z)=p_0+\rho g\,(z_0-z)\), where \(p_0\) is the pressure at height \(z_0\). The pressure at a point depends only on its depth below the free surface, not on the shape or width of the vessel.

Hence the force on the base of a vessel equals \(p\cdot(\text{base area})\), which can be far more or far less than the weight of the water in it. That is the hydrostatic paradox, discussed by Simon Stevin and Blaise Pascal. Pascal’s treatise on the equilibrium of liquids, published in 1663 after his death, argued partly from experiments that could hardly be performed, such as men sitting twenty feet under water. Boyle admired the reasoning but insisted on experiments that he and others had actually done.

Specific gravity by double weighing

By Archimedes’ principle a body immersed in water is buoyed up by the weight of the water it displaces. If a body weighs \(W_a\) in air and \(W_w\) when suspended in water, the displaced water weighs \(W_a-W_w\), so

\[ \mathrm{SG} = \frac{\rho}{\rho_{\text{water}}} = \frac{W_a}{W_a-W_w}. \]
Proposition (two-component mixture)

If an alloy of mass \(m\) consists of masses \(m_1, m_2\) of metals with densities \(\rho_1,\rho_2\), and volumes add, then its density \(\rho\) satisfies \(\dfrac{1}{\rho}=\dfrac{x}{\rho_1}+\dfrac{1-x}{\rho_2}\), where \(x=m_1/m\). Hence \(x=\dfrac{1/\rho-1/\rho_2}{1/\rho_1-1/\rho_2}\).

Exercise 6.1Torricelli’s mercury column is 0.760 m. How tall would a water barometer be? Boyle and Hooke heard that Pascal and others had raised water columns above 30 feet; does this agree?

Show solution
Equal pressures: \(\rho_w h_w=\rho_{\mathrm{Hg}}h_{\mathrm{Hg}}\), so \(h_w=13.595\times0.760\approx10.3\) m, about 34 feet. A water column of 30-odd feet is just what the weight of the air should hold up.

Exercise 6.2A coin weighs 20.00 g in air and 18.85 g in water. Gold has specific gravity 19.3 and silver 10.5. What is its specific gravity, and what fraction of its mass is gold, assuming it is a gold–silver alloy?

Show solution
\(\mathrm{SG}=20.00/1.15=17.39\). Then \(x=\dfrac{1/17.39-1/10.5}{1/19.3-1/10.5}=\dfrac{0.05750-0.09524}{0.05181-0.09524}=\dfrac{-0.03774}{-0.04343}\approx0.869\). About 87% gold by mass. Note that a 0.01 g error in the wet weighing changes the answer by about one percentage point, which is why Boyle cared about good balances.
Lesson 07

The Sceptical Chymist: what is an element?

For the general reader. In 1661 most learned people believed that everything was made of four elements (earth, water, air and fire) or of the three “principles” of the chemists (salt, sulphur and mercury). Boyle asked how anyone knew. When you burn wood you get ash, water, smoke and flame, but did those things exist inside the wood, or did the fire make them? His book is an argument that chemistry must rest on experiment, and it gave the operational idea of an element that chemists later used.

Goals
  • Follow Boyle’s arguments against fire as a universal analyser.
  • State his definition of an element and compare it with Lavoisier’s.
  • Use a mass balance to test a claim about composition.

The dialogue

The Sceptical Chymist is a conversation in a garden. Carneades, the sceptic, speaks largely for Boyle; Themistius defends Aristotle’s four elements; Philoponus defends the chemists’ three principles, derived from Paracelsus; Eleutherius moderates. Carneades argues that:

  • fire does not merely separate pre-existing ingredients; it can produce new substances, as when sand and alkali fuse into glass, which no one claims was hidden in either;
  • different methods of analysis yield different numbers and kinds of products from the same body, so the number of elements cannot be read off from analysis by fire;
  • some bodies, such as gold, cannot be decomposed by fire at all, which would make them elements on the chemists’ own test.
Boyle’s definition (1661), paraphrased

Elements are certain primitive and simple bodies, not made of any other bodies or of one another, which are the ingredients of which all perfectly mixed bodies are compounded and into which they are ultimately resolved.

Having stated this, Carneades doubts that any such bodies have been shown to exist. Boyle was a corpuscularian (Lesson 08): he thought all matter was one universal stuff, differentiated by the size, shape and motion of its particles. The definition was a tool to clear away the old systems, not a list. More than a century later Antoine Lavoisier made it operational: an element is a substance that has not yet been decomposed by any means of analysis. His 1789 list had 33 entries, including light and caloric.

The willow tree

Boyle discussed Jan Baptist van Helmont’s experiment with a willow, which seemed to show that water could be turned into wood and so was the one true element. Van Helmont planted a 5-pound willow in 200 pounds of dried earth and gave it only rainwater. After five years the tree weighed about 169 pounds, while the earth had lost only about 2 ounces. Boyle repeated growth experiments with plants in water and took them seriously as evidence that substances transform.

Exercise 7.1From van Helmont’s numbers, what fraction of the willow’s gain could have come from the soil? Which input did he and Boyle leave out of the mass balance, and roughly how much carbon does the gain represent if dry wood is about 50% carbon and the fresh tree about 50% water?

Show solution
Gain about 164 lb; soil lost 2 oz = 0.125 lb, under 0.1% of the gain. The missing input is carbon dioxide from the air, fixed by photosynthesis (with water supplying hydrogen and the oxygen released). Dry mass about 82 lb, carbon about 41 lb, all of it from atmospheric CO₂. Van Helmont, who named “gas”, had no way to weigh it.

Exercise 7.2Sand (SiO₂) fused with soda (Na₂CO₃) gives glass and a gas. Write a simplified equation for forming sodium silicate, and explain why this example supports Carneades’ argument about fire.

Show solution
\(\mathrm{SiO_2+Na_2CO_3\to Na_2SiO_3+CO_2}\). The glass is a new compound produced by the heat; it was not present in either starting material. So the products of fire need not be the “ingredients” of the bodies heated, which is exactly Carneades’ point.
Lesson 08

Corpuscles, qualities and the kinetic theory

For the general reader. Boyle thought the world was a machine made of tiny particles. Colour, heat, taste and smell were not separate things in objects but effects of the particles’ size, shape, motion and arrangement on our senses. He could not see the particles, but he could show that his machine-picture explained experiments. Seventy-six years after his law, Daniel Bernoulli showed how particles in motion produce exactly that law.

Goals
  • State Boyle’s “mechanical affections” and the distinction later called primary and secondary qualities.
  • Compare Boyle’s two models of the spring of the air.
  • Derive \(pV=\tfrac13 Nm\langle v^2\rangle\) and recover Boyle’s law.

The corpuscular philosophy

Boyle coined the phrase “corpuscular philosophy” and used it interchangeably with “mechanical philosophy”. In The Origin of Forms and Qualities (1666) he argued that matter is one and the same everywhere, and that bodies differ only in the size, shape and motion of their parts and their arrangement, which he called the mechanical affections of matter. Other qualities, such as colour and heat, arise from these together with the structure of our sense organs. John Locke, Boyle’s friend, made the terms primary and secondary qualities standard. Boyle avoided committing himself to Descartes’ plenum or to Gassendi’s atoms in the void; he wanted a framework that experiments could fill in.

Two pictures of the spring

In 1660 Boyle offered two possible explanations of the air’s elasticity without choosing between them. In the first, the particles of air are like tiny springs, or like a fleece of wool, that resist being pressed together. In the second, following Descartes, the particles are kept in rapid whirling motion by a subtle fluid and fly apart when given room. The second is closer to the explanation that won.

Bernoulli’s derivation (1738)

In Hydrodynamica Daniel Bernoulli modelled a gas as many small particles moving rapidly and bouncing off the walls. In modern form: let \(N\) particles of mass \(m\) move in a cube of side \(L\). A particle with velocity component \(v_x\) hits a given wall every \(2L/|v_x|\) and transfers momentum \(2m|v_x|\) each time.

Theorem (kinetic pressure)

For an ideal gas of \(N\) point particles in volume \(V\), with isotropic velocities and elastic wall collisions, \(\displaystyle pV=\tfrac13Nm\langle v^2\rangle=\tfrac23E_{\mathrm{kin}}\). Hence at fixed mean kinetic energy, that is, fixed temperature, \(pV\) is constant.

Derivation. The average force on one wall of area \(L^2\) is \(\sum_i 2m v_{x,i}^2/(2L)=Nm\langle v_x^2\rangle/L\), so \(p=Nm\langle v_x^2\rangle/L^3\). Isotropy gives \(\langle v_x^2\rangle=\tfrac13\langle v^2\rangle\). Comparing with \(pV=Nk_BT\) identifies \(\tfrac12m\langle v^2\rangle=\tfrac32k_BT\). Bernoulli also saw that compressing the gas faster than heat can escape would raise the speeds and the pressure, the adiabatic correction to Boyle’s law.

Exercise 8.1Find the root-mean-square speed of nitrogen molecules (molar mass 28.0 g/mol) at 288 K. Compare with the speed of sound in air, about 340 m/s.

Show solution
\(v_{\mathrm{rms}}=\sqrt{3RT/M}=\sqrt{3\times8.314\times288/0.0280}=\sqrt{2.566\times10^5}\approx507\) m/s. The speed of sound is somewhat lower, \(\sqrt{\gamma RT/M}\approx346\) m/s with \(\gamma=1.4\). Sound is carried by the same molecular motion, so the two must be comparable.

Exercise 8.2Show from the kinetic theorem that if a gas is compressed slowly at constant temperature to half its volume, the number of molecular impacts per second on each square centimetre of wall doubles. Why is this a more satisfying account of Boyle’s law than the fleece of wool?

Show solution
The impact rate per unit area is \(\tfrac14 n\langle |v|\rangle\) with \(n=N/V\) the number density. At fixed \(T\), \(\langle|v|\rangle\) is fixed and \(n\) doubles, so the rate doubles, and with it the momentum flux, the pressure. The kinetic model predicts the exact exponent \(-1\) from mechanics alone, and it ties pressure to temperature. A fleece of springs would need a special force law to give exactly \(p\propto1/V\), and it says nothing about heating.
Lesson 09

Fire, air, phosphorus and indicators

For the general reader. Boyle showed that a candle and a mouse both die in an exhausted receiver, and he found that metals gain weight when they are heated in air. He made a new “factitious air” that burned, prepared the glowing substance phosphorus, and used plant juices that change colour to tell acids from alkalis. He drew the wrong conclusion about the weight gain, and the story of how it was corrected leads straight to Lavoisier.

Goals
  • Analyse the calcination of metals with a mass balance.
  • Compute the gas produced when iron dissolves in acid.
  • Explain colour indicators by an acid–base equilibrium.

Calcination and the fire particles

When tin or lead is heated strongly in air it turns into a powdery calx that weighs more than the metal. Boyle heated metals in sealed glass retorts, broke them open, and weighed the products. He found the gain and, in work published in 1673, attributed it to particles of fire that passed through the glass and fixed themselves in the metal. Lavoisier in 1774 repeated the experiment with tin in a sealed vessel and weighed the whole vessel before and after. Its total weight did not change. When the vessel was opened, air rushed in, and the weight of that air equalled the gain of the tin. Boyle had weighed the calx after air had entered.

Conservation of mass in a closed system

In a sealed vessel, the total mass is unchanged by any chemical reaction inside it. A gain in mass of one product must be balanced by a loss from another component, here the oxygen of the enclosed air: \(\mathrm{Sn+O_2\to SnO_2}\).

Factitious air, flame and life

Boyle dissolved iron filings in dilute acid and collected an air that burned; we call it hydrogen. His 1660 experiments showed that flame and animal life both require air, and that a small animal in a closed vessel dies as the air is “spent”, long before it is all used up. Later he described a viper placed in an exhausted receiver with a bubble visible in the fluid of its eye, the first recorded description of decompression sickness.

Phosphorus

The Hamburg alchemist Hennig Brand obtained white phosphorus from urine in 1669. The secret was sold to Johann Daniel Kraft, who demonstrated it in London, where Boyle saw it. Boyle worked out a preparation for himself and in 1680 published his method, together with observations of its cold glow in air. He was the first to use phosphorus to ignite splints tipped with sulphur, ancestors of the match. His assistant Ambrose Godfrey later made a business of manufacturing phosphorus.

Indicators

In Experiments and Considerations Touching Colours (1664) Boyle reported that syrup of violets and other plant extracts turn one colour with acids and another with alkaline salts, and he proposed such colour changes as a test to sort substances into acid, alkaline and neither. This was a precursor of litmus paper. The modern explanation: the dye is a weak acid \(\mathrm{HIn}\) whose two forms have different colours.

\[ \mathrm{HIn \rightleftharpoons H^+ + In^-},\qquad \mathrm{pH}=\mathrm{p}K_a+\log_{10}\frac{[\mathrm{In^-}]}{[\mathrm{HIn}]}. \]

Exercise 9.110.00 g of tin (molar mass 118.71 g/mol) is fully calcined to SnO₂ in a sealed 2.00 L flask of air at 1 atm and 288 K. Air is 21% oxygen by volume. Is there enough oxygen? By how much does the solid gain in mass, and what happens to the total mass of the flask?

Show solution
Tin: \(10.00/118.71=0.0842\) mol, needing 0.0842 mol O₂. The flask holds \(n=pV/RT=101325\times0.002/(8.314\times288)=0.0846\) mol of air, of which 0.0178 mol is O₂. So oxygen runs out first: only 0.0178 mol O₂ reacts, the solid gains \(0.0178\times32.00=0.57\) g, and about 21% of the tin is converted. The total mass of the sealed flask is unchanged; on opening, about 0.57 g of air rushes in. Boyle’s full calcinations needed far more air than any sealed flask holds, which hid this bookkeeping.

Exercise 9.2Iron (55.85 g/mol) dissolves in hydrochloric acid: \(\mathrm{Fe+2HCl\to FeCl_2+H_2}\). What volume of hydrogen at 1 atm and 288 K comes from 5.585 g of iron?

Show solution
0.1000 mol Fe gives 0.1000 mol H₂. \(V=nRT/p=0.1\times8.314\times288/101325=2.36\times10^{-3}\ \mathrm{m^3}\), about 2.4 litres.

Exercise 9.3The eye sees a clear change of colour when the ratio of the two forms of an indicator passes from about 1:10 to 10:1. Over what pH range does an indicator with \(\mathrm pK_a=7.0\) change? What fraction is in the basic form at pH 8?

Show solution
From \(\mathrm{pH}=\mathrm pK_a\pm1\): pH 6 to 8. At pH 8, \([\mathrm{In^-}]/[\mathrm{HIn}]=10\), so the basic fraction is \(10/11\approx91\%\).
Lesson 10

Beyond the ideal: the Boyle temperature

For the general reader. Boyle’s law is exact only for an imaginary gas whose molecules have no size and do not attract each other. Real gases deviate. Molecules attract at a distance, which lowers the pressure, and they take up room, which raises it. At one special temperature, named the Boyle temperature, the two effects cancel and a real gas obeys Boyle’s law over a wide range of pressures.

Goals
  • Write the virial expansion and interpret the second virial coefficient.
  • Derive the Boyle temperature of a van der Waals gas.
  • Show that Boyle’s own data could not have detected the deviation.

The virial expansion

For a real gas, the compressibility factor \(Z=pV_m/RT\) can be expanded in powers of the molar density:

\[ Z = 1 + \frac{B(T)}{V_m} + \frac{C(T)}{V_m^2} + \cdots, \qquad\text{equivalently}\qquad Z = 1 + \frac{B(T)\,p}{RT} + O(p^2). \]

The second virial coefficient \(B(T)\) comes from interactions between pairs of molecules. It is negative at low temperature, where attraction dominates, and positive at high temperature, where the excluded volume dominates.

Definition and theorem (Boyle temperature)

The Boyle temperature \(T_B\) is the temperature at which \(B(T_B)=0\), so that \(\big(\partial Z/\partial p\big)_T=0\) at \(p=0\) and \(pV\) is constant to first order in \(p\). For the van der Waals equation \(\big(p+\tfrac{a}{V_m^2}\big)(V_m-b)=RT\), one has \(B(T)=b-\dfrac{a}{RT}\), hence

\[ T_B=\frac{a}{Rb}=\frac{27}{8}\,T_c, \qquad T_c=\frac{8a}{27Rb}. \]

Derivation. Solve for \(p=\dfrac{RT}{V_m-b}-\dfrac{a}{V_m^2}\) and expand \(\dfrac{1}{V_m-b}=\dfrac{1}{V_m}\big(1+\tfrac{b}{V_m}+\cdots\big)\). Then \(Z=1+\dfrac{1}{V_m}\Big(b-\dfrac{a}{RT}\Big)+O(V_m^{-2})\). The critical temperature follows from the inflection conditions \(\partial p/\partial V_m=\partial^2p/\partial V_m^2=0\).

Exercise 10.1For nitrogen, \(a=1.370\ \mathrm{L^2\,bar\,mol^{-2}}\) and \(b=0.0387\ \mathrm{L\,mol^{-1}}\). Compute the van der Waals Boyle temperature. The measured value is about 327 K. Comment.

Show solution
\(T_B=a/(Rb)=1.370/(0.08314\times0.0387)\approx426\) K. The van der Waals model overestimates by about 30%, a typical size of error for a two-parameter model fitted at the critical point. The qualitative picture, attraction against excluded volume, is right.

Exercise 10.2At room temperature air has \(B\approx-8\ \mathrm{cm^3\,mol^{-1}}\). Estimate the relative deviation of \(pV\) from its low-pressure value at four atmospheres, the highest pressure in Boyle’s table, and compare with his scatter of about 0.7%.

Show solution
\(Z-1\approx Bp/RT=(-8\times10^{-6})(4.05\times10^5)/(8.314\times290)\approx-1.3\times10^{-3}\), about 0.13%. This is five times smaller than the scatter in Boyle’s data, so his experiment could not have detected it. Real-gas deviations were first measured reliably by Henri Victor Regnault in the 1840s.
Part III · Life and legacy
Lesson 11

Pall Mall and the Royal Society, 1668–1691

In 1668 Boyle moved to London and lived for the rest of his life in his sister Katherine’s house in Pall Mall, where he built a laboratory. Visitors came to see experiments and to consult him. His health had never been strong. In June 1670 he suffered a stroke that left him paralysed for a time. He recovered slowly, cut back his public engagements, and kept writing, often by dictation to secretaries, at an enormous rate.

He remained the Royal Society’s most celebrated experimental Fellow. His papers filled the early Philosophical Transactions, and his presence lent the Society the respectability of a pious, aristocratic gentleman. In 1680 the Fellows elected him President. He declined, explaining that he had scruples about taking the oaths required by the charter. Christopher Wren was elected in his place.

Chymistry and alchemy

Boyle’s chemistry included what historians now call chymistry: work on the transmutation of metals that we would classify as alchemy. He believed that a properly prepared mercury could act on gold, and he lobbied successfully for the repeal of the medieval statute that forbade the multiplication of gold and silver. Lawrence Principe’s studies of his manuscripts have shown how central this work was to him. It belongs to the same project as his corpuscular philosophy: if all matter is one stuff differently arranged, then rearrangement into gold is not absurd. Isaac Newton, who shared these interests, corresponded with him, including a long letter on the aether in 1679.

Religion and the wider world

Boyle saw experimental philosophy as a form of worship: the “Christian virtuoso” studied the creation to know the creator. A Free Enquiry into the Vulgarly Received Notion of Nature (1686) attacked the idea of Nature as a quasi-intelligent agent, arguing that the world is a mechanism whose laws God made and sustains. He was governor of the Corporation for the Propagation of the Gospel in New England and a director of the East India Company, and he paid for translations and printings of the Bible, including the Bible in Irish in the 1680s. He also employed and trained assistants who became natural philosophers in their own right, among them the Frenchman Denis Papin, who worked on the air pump with him in the later 1670s and went on to invent the steam digester.

DiscussionBoyle insisted on reporting failed experiments and on naming witnesses. Shapin and Schaffer argue that this “literary technology” was as important as the air pump itself. What modern practices in scientific publishing descend from it, and what problems does it not solve?

Lesson 12

Death, the Boyle Lectures and legacy

Katherine, Lady Ranelagh, died in December 1691. A week later, on 31 December 1691, Robert Boyle died in her house in Pall Mall, aged 64. He was buried in the chancel of St Martin-in-the-Fields; the church was rebuilt in the eighteenth century and the grave is lost. Gilbert Burnet, Bishop of Salisbury, preached the funeral sermon. John Locke saw his unfinished General History of the Air through the press in 1692.

His will endowed a series of eight sermons a year to defend Christianity against unbelievers, without entering into controversies among Christians. Richard Bentley gave the first Boyle Lectures in 1692, drawing on Newton’s Principia and corresponding with Newton about it. The lectures were revived in 2004 and continue in London.

Legacy

  • Physics: the law \(pV=\text{const}\), the first quantitative law of a gas, and the first step to the ideal gas law and kinetic theory. The Boyle temperature of real gases bears his name.
  • Chemistry: the critique of the four elements and three principles, the operational spirit later made precise by Lavoisier, careful analysis by reagents and indicators, and the separation of chemistry from medicine as a subject in its own right.
  • Method: detailed, repeatable reporting of experiments; the use of instruments to produce new phenomena; the idea that matters of fact are established by witnessed trials. These practices shaped the Royal Society and modern experimental science.
  • Honours: the Royal Dublin Society’s Boyle Medal, first awarded in 1899, and the Royal Society of Chemistry’s Robert Boyle Prize for Analytical Science.

Final projectChoose one experiment from New Experiments (1660). Describe it as Boyle did, then analyse it with the physics of Part II: what was measured, what modern quantities explain it, and whether Boyle’s apparatus could have detected the effect he claimed.

Reference

Connections

People linked to Robert Boyle across this collection. A name without a link has no page here yet. See Robert Boyle in the network of all 337 lives →

Influenced by

Influenced

Colleagues and collaborators

Rivals

  • Franciscus Linus 1661-1662
  • Thomas Hobbes 1661-1674

Friends

  • John Locke

Family

  • Katherine Jones, Viscountess Ranelagh

Also mentioned in this life

Fields

Reference

Sources and further reading

Biography

  1. J. J. O’Connor and E. F. Robertson, Robert Boyle, MacTutor History of Mathematics.
  2. Robert Boyle, Wikipedia.
  3. J. J. MacIntosh and P. Anstey, Robert Boyle, Stanford Encyclopedia of Philosophy.
  4. M. Hunter, Boyle: Between God and Science, Yale University Press, 2009.
  5. S. Shapin and S. Schaffer, Leviathan and the Air-Pump: Hobbes, Boyle, and the Experimental Life, Princeton University Press, 1985.
  6. L. M. Principe, The Aspiring Adept: Robert Boyle and His Alchemical Quest, Princeton University Press, 1998.
  7. Linda Hall Library, Scientist of the Day: Robert Boyle.

Physics and chemistry

  1. R. Boyle, New Experiments Physico-Mechanicall, Touching the Spring of the Air, and its Effects, Oxford, 1660; 2nd ed. with A Defence of the Doctrine touching the Spring and Weight of the Air, 1662.
  2. R. Boyle, The Sceptical Chymist, London, 1661. Project Gutenberg text.
  3. R. Boyle, Experiments and Considerations Touching Colours, London, 1664. Project Gutenberg text.
  4. R. Boyle, Hydrostatical Paradoxes, Oxford, 1666; Medicina Hydrostatica, London, 1690.
  5. M. Hunter and E. B. Davis (eds.), The Works of Robert Boyle, 14 vols., Pickering & Chatto, 1999–2000.
  6. Boyle’s 1662 compression table, transcribed at ChemTeam.
  7. Boyle’s law and The Sceptical Chymist, Wikipedia.
  8. D. Bernoulli, Hydrodynamica, Strasbourg, 1738, section X (kinetic theory of gases).