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Physics 1785

First Memoir on Electricity and Magnetism

Charles-Augustin de Coulomb

Two charges push or pull as the inverse square of their distance — electricity gets its first exact law.

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In depth · the introduction

How hard do two specks of static electricity push on each other — and how fast does that push fade as you pull them apart? In 1785 Coulomb built a balance delicate enough to weigh the answer.

The idea

Rub a balloon on your hair and it crackles; two charged objects plainly push or pull on each other. But by how much? Coulomb pinned it to a clean rule. The force depends on two things: how much charge each object carries, and how far apart they are. More charge means more force. And distance matters enormously — move the objects twice as far apart and the force doesn't just halve, it drops to a quarter; three times as far, to a ninth. That steep fade is called an inverse-square law.

It was the very same shape Newton had found for gravity a century earlier — and that was the thrilling part. The silent pull of gravity and the crackle of static electricity, two utterly different forces, turned out to obey mathematics of exactly the same form.

How he measured it

Forces between little charged balls are far too feeble for an ordinary scale, so Coulomb built one of the most sensitive instruments of his age: the torsion balance. He hung a light arm from a long, fine silver wire, with a small charged ball on the end. When he brought a second charged ball close, the first was pushed away and the wire twisted — and a stronger push twisted it more. By reading the twist, he could weigh a force thousands of times too small to feel. He set the balls at a certain distance, then half of it, then a quarter, and watched the force climb in the tell-tale 1, 4, 16 pattern of an inverse square.

Why it mattered

Before Coulomb, electricity was a parlour curiosity — sparks, shocks and crackles with no numbers attached. He turned it into a measured science with a law you could calculate. That law is the reason atoms hold together: electrons are bound to their nuclei by exactly this force, so it quietly underlies all of chemistry, and every battery, screen and circuit you own. And by echoing Newton's law of gravity so precisely, it whispered that the forces of nature might share one deep design.

A picture

Think of the light from a single candle spreading into the dark. Step twice as far away and the candle looks a quarter as bright; three times as far, a ninth. The same fixed amount of light is being smeared over a bigger and bigger sphere as it travels outward. Electric force thins out with distance in exactly the same way, and for a related reason — it reaches out from a charge into all the space around it. That shared inverse-square fingerprint quietly links electricity, gravity, sound and light.

Two charged balls on a line: a fixed positive charge on the left and a second charge on the right. One slider sets the second charge from negative to positive — alike charges show red arrows pushing apart, opposite charges show blue arrows pulling together. A second slider sets the distance, and a curve plots how the force falls off as the inverse square of the distance.

Where it sits

Coulomb took the mathematical machinery Newton had built for gravity (see newton-1687) and showed it fit electricity too. His law became the bedrock on which the nineteenth century raised the rest: Faraday's lines of force (see faraday-1831), Ohm's law of the current (see ohm-1827), and at last Maxwell's union of electricity, magnetism and light (see maxwell-1865), where Coulomb's law reappears as the first of the four famous equations. The unit of electric charge is named the coulomb in his honour.

The original document
Original source text
Charles-Augustin de Coulomb · Premier mémoire sur l'électricité et le magnétisme · Histoire de l'Académie Royale des Sciences (1785), pp. 569–577
Coulomb opens by describing his instrument: a torsion balance in which a horizontal needle, charged at one end, hangs from a fine silver wire and is repelled by a second fixed charged ball, so that the electric force can be read off as the twist of the wire.
The fundamental law
La force répulsive de deux petits globes électrisés de la même nature d'électricité est en raison inverse du carré de la distance du centre des deux globes.
In the Assis–Bucciarelli translation: "The repulsive force of two small globes electrified with the same nature of electricity is inversely proportional to the square of the distance between the centers of the two globes."
The measurements
Three tabulated trials follow. Charged so that repulsion holds the needle about 36 degrees from the fixed ball, then disturbed so the balls sit roughly 18 and then about 8.5 degrees apart — halving and then quartering the separation — the wire must be twisted through forces close to the ratio 1 : 4 : 16, the signature of the inverse square.
[ … ]
Coulomb attributes the small departures from the exact law to a slow leakage of electricity from the balls during a run, and states that the attraction between opposite charges follows the same inverse-square form, which he confirms in the following memoir by timing the oscillations of a charged needle.
Paris · 1785