
French physicist best known for the formulation of Coulomb's law, which states that the force between two electrical charges is proportional to the product of the charges and inversely proportional to the square of the distance between them. Coulombic force is one of the principal forces involved in atomic reactions. 
Charles Augustin Coulomb's father was Henry Coulomb and his mother was Catherine Bajet. Both his parents came from families which were well known in their fields. His father's family were important in the legal profession and in the administration of the Languedoc region of France, and his mother's family were also quite wealthy. After being brought up in Angoulême, the capital of Angoumois in southwestern France, Coulomb's family moved to Paris. In Paris he entered the Collège Mazarin, where he received a good classical grounding in language, literature, and philosophy, and he received the best available teaching in mathematics, astronomy, chemistry and botany.
At this stage in his education there was a crisis for Coulomb. Despite his father's good standing, he had made unsuccessful financial speculations, had lost all his money and moved from Paris to Montpellier. Coulomb's mother remained in Paris but Coulomb had a disagreement with her over the direction his career should take so he left Paris and went to Montpellier to live with his father. At this stage Coulomb's interests were mainly in mathematics and astronomy and while in Montpellier he joined the Society of Sciences there in March 1757 and read several papers on these topics to the Society.
Coulomb wanted to enter the Ecole du Génie at Mézières but realised that to succeed in passing the entrance examinations he needed to be tutored. In October 1758 he went to Paris to receive the tutoring necessary to take the examinations. Camus had been appointed as examiner for artillery schools in 1755 and it was his Cours de mathématique that Coulomb studied for several months. In 1758 Coulomb took the examinations set by Camus which he passed and he entered the Ecole du Génie at Mézières in February 1760. He formed a number of important friendships around this time which were imporatnt in his later scientific work, one with Bossut who was his teacher at Mézières and the other with Borda.
Coulomb graduated in November 1761. He was now a trained engineer with
the rank of lieutenant in the Corps du Génie. Over the next twenty
years he was posted to a variety of different places where he was involved
in engineering, in structural design, fortifications, soil mechanics, and
many other areas. His first posting was to Brest but in February 1764 he
was set to Martinique in the West Indies. Martinique fell under the sovereignty
of France under Louis XIV in 1658. However Martinique was attacked by a
number of foreign fleets over the following years. The Dutch attacked it
in 1674 but were driven off, as were the English in 1693 and the English
again in 1759. Martinique was finally captured by the English in 1762 but
were returned to France under the terms of the Treaty of Paris in 1763.
The French then made attempts to make the island more secure by building
a new fort.

Coulomb was put in charge of the building of the new Fort Bourbon and this task occupied him until June 1772. It was a period during which he showed the practical side of his engineering skills which were needed to organise the construction, but his experiences would play a major role in the later theoretical memoirs he wrote on mechanics. As far as Coulomb's health was concerned these were difficult years and the illnesses which he suffered while on Martinique left him in poor health for the rest of his life. 
On his return to France, Coulomb was sent to Bouchain. However, he now began to write important works on applied mechanics and he presented his first work to the Académie des Sciences in Paris in 1773. This work, "Sur une application des règles, de maximis et minimis à quelque problèmes de statique, relatifs à l'architecture" was written (in Coulomb's words, see for example [1]):
" ... to determine, as far as a combination of mathematics and physics will permit, the influence of friction and cohesion in some problems of statics."
Perhaps the most significant fact about this memoir from a mathematical point of view is Coulomb's use of the calculus of variations to solve engineering problems. Coulomb wrote on structural analysis, the fracture of beams, the fracture of columns, the thrust of arches and the thrust of the soil. As Gillmor writes in [1]:
"In this one memoir of 1773 there is almost an embarrassment of riches, for Coulomb proceeded to discuss the theory of comprehensive rupture of masonry piers, the design of vaulted arches, and the theory of earth pressure. In the latter he developed a generalised sliding wedge theory of soil mechanics that remains in use today in basic engineering practice. A reason, perhaps, for the relative neglect of this portion of Coulomb's work was that he sought to demonstrate the use of variational calculus in formulating methods of approach to fundamental problems in structural mechanics rather than to give numerical solutions to specific problems."
It is often the case that a sophisticated use of mathematics in an application
to an area where most have less mathematical sophistication, gives the
work a long term values which is not often seen at the time. The memoir
was certainly highly valued by the Académie des Sciences for it
led to him being named as Bossut's correspondent on 6 July 1774. From Bouchain,
Coulomb was next posted to Cherbourg. While he was there he wrote a famous
memoir on the magnetic compass which he submitted for the Grand Prix of
the Académie des Sciences in 1777.

This 1777 paper won Coulomb a share of the prize and it contained his
first work on the torsion balance [1]: "... his simple,
elegant solution to the problem of torsion in cylinders and his use of
the torsion balance in physical applications were important to numerous
physicists in succeeding years. ... Coulomb developed a theory of torsion
in thin silk and hair threads. Here he was the first to show how the torsion
suspension could provide physicists with a method of accurately measuring
extremely small forces."

Coulomb's torsion balance 

Charles Augustin de Coulomb invented the torsin balance which could measure electrostatic force. Inside the balance are two pith balls. One is mounted and unmovable, the other can roll around. When the two pith balls are enegized by an electrostatic charge the moveable one will be roll away from the stationary one, if both receive the same type of charge (positive or negative). It will roll towards the stationary pith ball, if each receives a different charge. The distance it rolls is used to measure the electrostatic force. Coulomb was able to measure the torsion on the fiber with the scale near the top of the device and the distance between the balls on the scale that circumscribed the jar. He was able to derive a mathematical equation that described the relationship between these two variables. The force between two small, charged spheres is shown to be proportional to the magnitude of either charge and inversely proportional to the square of the distance between centers. This torsional balance device requires low humidity! 


Another interesting episode occurred during the time which Coulomb spent at Cherbourg. RobertJacques Turgot was appointed comptroller general by Louis XVI on 24 August 1774. He began to feel threatened by his political opponents in 1775 and began a series of reforms. Among these was the reform of the Corps du Génie and Turgot called for memoirs on its possible reorganisation. Coulomb submitted a memoir giving his ideas and it is a fascinating opportunity to understand his political views. Coulomb wanted the state and the individual to play equal roles. He proposed that the Corps du Génie in particular, and all public service in general, should recognise the talents of its individual members in promotion within the organisation.
In 1779 Coulomb was sent to Rochefort to collaborate with the Marquis de Montalembert in constructing a fort made entirely from wood near Ile d'Aix. Like Coulomb, the Marquis de Montalembert had a reputation as a military engineer designing fortifications, but his innovative work had been criticised by many French engineers [2]:
"Viewing fortresses as nothing more than immense permanent batteries designed to pour overwhelming fire on attacking armies, Montalembert simplified the intricate geometric designs of Vauban and relied on simple polygonal structures, often with detached peripheral forts instead of projecting bastions."
During his time at Rochefort, Coulomb carried on his research into mechanics, in particular using the shipyards in Rochefort as laboratories for his experiments. He also did research on friction of machinery, on windmills, and on the elasticity of metal and silk fibres. His studies into friction in Rochefort led to Coulomb's major work on friction Théorie des machines simples which won him the Grand Prix from the Académie des Sciences in 1781. In this memoir Coulomb [1]:
"... investigated both static and dynamic friction of sliding surfaces and friction in bending of cords and in rolling. From examination of many physical parameters, he developed a series of twoterm equations, the first term a constant and the second term varying with time, normal force, velocity, or other parameters."
Because of this prize winning work, the authors of [5] write:
"Coulomb's contributions to the science of friction were exceptionally great. Without exaggeration, one can say that he created this science."
In fact this 1781 memoir changed Coulomb's life. He was elected to the mechanics section of the Académie des Sciences as a result of this work, and he moved to Paris where he now held a permanent post. He never again took on any engineering projects, although he did remain as a consultant on engineering matters, and he devoted his life from this point on to physics rather than engineering. Coulomb developed his law as an outgrowth of his attempt to investigate the law of electrical repulsions as stated by Joseph Priestley of England. To this end he invented sensitive apparatus to measure the electrical forces involved in Priestley's law. He also established the inverse square law of attraction and repulsion of unlike and like magnetic poles, which became the basis for the mathematical theory of magnetic forces developed by SiméonDenis Poisson. He wrote seven important treatises on electricity and magnetism which he submitted to the Académie des Sciences between 1785 and 1791. These seven papers are discussed in [6] where the author shows that Coulomb:
"... had obtained some remarkable results by using the torsion balance method: law of attraction and repulsion, the electric point charges, magnetic poles, distribution of electricity on the surface of charged bodies and others. The importance of Coulomb's law for the development of electromagnetism is examined and discussed."
In these he developed a theory of attraction and repulsion between bodies of the same and opposite electrical charge. He demonstrated an inverse square law for such forces and went on to examine perfect conductors and dielectrics. He suggested that there was no perfect dielectric, proposing that every substance has a limit above which it will conduct electricity. These fundamental papers put forward the case for action at a distance between electrical charges in a similar way as Newton's theory of gravitation was based on action at a distance between masses.
These papers on electricity and magnetism, although the most important of Coulomb's work over this period, were only a small part of the work he undertook. He presented twentyfive memoirs to the Académie des Sciences between 1781 and 1806. Coulomb worked closely with Bossut, Borda, de Prony, and Laplace over this period. Remarkably he participated in the work of 310 committees of the Academy. He still was involved with engineering projects as a consultant, the most dramatic of which was his report on canal and harbour improvements in Brittany in 178384. He had been pressed into this task against his better judgement and he ended up taking the blame when criticisms were made and he spent a week in prison in November 1783.
He also undertook services for the respective French governments in such varied fields as education and reform of hospitals. In 1787 he made a trip to England to report on the conditions in the hospitals of London. In July 1784 he was appointed to look after the royal fountains and took charge of a large part of the water supply of Paris. On 26 February 1790 Coulomb's first son was born, although he was not married to Louise Françoise LeProust Desormeaux who was the mother of his son.
When the French Revolution began in 1789 Coulomb had been deeply involved with his scientific work. Many institutions were reorganised, not all to Coulomb's liking, and he retired from the Corps du Génie in 1791. At about the same time that the Académie des Sciences was abolished in August 1783, he was removed from his role in charge of the water supply and, in December 1793, the weights and measures committee on which he was serving was also disbanded. Coulomb and Borda retired to the country to do scientific research in a house he owned near Blois.
The Académie des Sciences was replaced by the Institut de France and Coulomb returned to Paris when he was elected to the Institute in December 1795. On 30 July 1797 his second son was born and, in 1802, he married Louise Françoise LeProust Desormeaux, the mother of his two sons. We mentioned above that Coulomb was involved with services to education. These were largely between 1802 and 1806 when he was inspector general of public instruction and, in that role, he was mainly responsible for setting up the lycées across France.
Let us end with quoting the tribute paid to him by Biot who wrote:
"It is to Borda and to Coulomb that one owes the renaissance of true
physics in France, not a verbose and hypothetical physics, but that ingenious
and exact physics which observes and compares all with rigour."



Coulomb force also called COULOMB INTERACTION, attraction or repulsion of particles or objects because of their electric charge. One of the basic physical forces, the electric force is named for a French physicist, CharlesAugustin de Coulomb, who in 1785 published the results of an experimental investigation into the correct quantitative description of this force.
Two like electric charges, both positive or both negative, repel each other along a straight line between their centres. Two unlike charges, one positive, one negative, attract each other along a straight line joining their centres. The electric force is operative between charges down to distances of at least 10^{16} m, or approximately onetenth of the diameter of atomic nuclei. Because of their positive charge, protons within nuclei repel each other, but nuclei hold together because of another basic physical force, the strong interaction, or nuclear force, which is stronger than the electric force. Massive, but electrically neutral, astronomical bodies such as planets and stars are bound together in solar systems and galaxies by still another basic physical force, gravitation, which though much weaker than the electric force, is always attractive and is the dominant force at great distances. At distances between these extremes, including the distances of everyday life, the only significant physical force is the electric force in its many varieties along with the related magnetic force.
The magnitude of the electric force F is directly proportional to the amount of one electric charge, q_{1}, multiplied by the other, q_{2}, and inversely proportional to the square of the distance r between their centres. Expressed in the form of an equation, this relation, called Coulomb's law, may be written by including the proportionality factor k as F = k(q_{1}q_{2})/r^{2}. In the centimetregramsecond system of units, the proportionality factor k in a vacuum is set equal to 1 and unit electric charge is defined by Coulomb's law. If an electric force of one unit (one dyne) arises between two equal electric charges one centimetre apart in a vacuum, the amount of each charge is one electrostatic unit, esu, or statcoulomb. In the metrekilogramsecond and the SI systems, the unit of force (newton), the unit of charge (coulomb), and the unit of distance (m), are all defined independently of Coulomb's law, so the proportionality factor k is constrained to take a value consistent with these definitions, namely, k in a vacuum equals 8.98x10^{9} newton square metre per square coulomb. This choice of value for k permits the practical electrical units, such as ampere and volt, to be included with the common metric mechanical units, such as metre and kilogram, in the same system.
Coulombic potential energy can be derived from the above formulated equation of the Coulombic force:
The coulomb, a unit of electric
charge, was named in his honour. In the metre  kilogram  second  ampere
system, the basis of the SI system of physical units, the coulomb is defined
as the quantity of electricity transported in one second by a current of
one ampere. It is approximately equivalent to 6.24x10^{18}
electrons.
1. Biography in Dictionary of Scientific Biography (New
York 19701990).
2. Biography in Encyclopaedia Britannica.
Books:
3. C S Gillmor, Charles Augustin Coulomb : Physics and Engineering
in Eighteenth Century
France (Princeton, N.J., 1971).
Articles:
4. S B Hamilton, Charles Auguste de Coulomb, Trans. Newcomen Soc.
(London) 17 (1938),
2749.
5. I V Kragelskii and V S Schedrov, in: Development
of the science of friction  dry friction
(Moscow, 1956), 5169.
6. Yu A Lyubimov, The memoirs of Coulomb  the beginning
of modern electromagnetism
(Russian), in: History and methodology of the
natural sciences, (Moscow, 1983), 101129.