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Atlas / Physics / The Relativity Thread

Field · Emerged 1820 – 1865

Electromagnetism

How are electricity, magnetism and light connected?

5 chapters4 min read5 turning points1 open problem

Branched from
One of the thread's roots
Branched into
Astronomical Spectroscopy + Crystallography + Old Quantum Theory + Radioactivity + Special Relativity + Wave Optics
Figures
Hans Christian Ørsted, Michael Faraday, Joseph Henry, James Clerk Maxwell, Heinrich Hertz, Albert Michelson, Edward Morley, Hendrik Lorentz

In brief

Electromagnetism is the physics of electric charges, currents and magnets, and of the light and radio waves they produce. Over the nineteenth century, three phenomena that looked unrelated (static sparks, compass needles and light) turned out to be one thing: an electromagnetic field filling space, whose ripples travel at the speed of light.

It powers the modern world, from generators to Wi-Fi. It also set the stage for relativity. Maxwell's equations fix a single speed of light, and nothing in Newton's mechanics could accommodate that.

Key ideas

FieldEnters 1831

Faraday's idea that charges and magnets fill the space around them with something real, lines of force, that acts on other charges. Forces are no longer mysterious actions at a distance.

Electromagnetic inductionEnters 1831

A changing magnetic field produces an electric current. Every generator, transformer and induction hob works this way.

Maxwell's equationsEnters 1861 – 1865

Four equations that describe how charges and currents create electric and magnetic fields, and how changing fields create each other. All classical electromagnetism follows from them.

The speed of lightEnters 1861 – 1865

Maxwell's equations predict waves travelling at c=1/μ0ε0c = 1/\sqrt{\mu_0 \varepsilon_0}, a speed fixed by two constants measured with coils and capacitors. It matched the measured speed of light, so light is an electromagnetic wave.

The etherEnters 1887

The medium that light waves were assumed to travel through, as sound travels through air. Measurements of the Earth's motion through it kept coming out zero.

Draws on other domains

Chapter I

Two Forces, One Needle

For most of history, electricity and magnetism were separate curiosities. Magnets pointed north, amber rubbed with fur attracted straw, and lightning was a mystery until Franklin tied it to sparks. By 1785 Coulomb had shown that electric charges attract and repel with an inverse-square law, just like Newton's gravity, and it was natural to think of electricity as another force acting at a distance.

In 1820 Hans Christian Ørsted noticed a compass needle twitch beside a wire carrying current. An electric current makes magnetism. Within months Ampère in Paris had measured the forces between currents, and the two subjects began to merge.

Chapter II

Faraday's Lines

Michael Faraday, a bookbinder's apprentice turned experimenter with almost no mathematics, asked the reverse question: can magnetism make electricity? In 1831 he found that it can, but only when something changes. Switching a current on in one coil, or moving a magnet through another, drives a brief current. Joseph Henry in Albany found the same effect independently.

To think about it, Faraday imagined space around magnets and charges filled with lines of force, visible in the patterns iron filings make. Most physicists treated the lines as a picture. Faraday insisted they were real, and that the space between objects is where the physics happens. The field was the most consequential idea of the century.

Chapter III

Maxwell's Light

James Clerk Maxwell turned Faraday's pictures into mathematics. In modern notation, his equations say:

∇⋅E=ρε0,∇⋅B=0,∇×E=−∂B∂t,∇×B=μ0J+μ0ε0∂E∂t.\nabla \cdot \mathbf{E} = \frac{\rho}{\varepsilon_0}, \quad \nabla \cdot \mathbf{B} = 0, \quad \nabla \times \mathbf{E} = -\frac{\partial \mathbf{B}}{\partial t}, \quad \nabla \times \mathbf{B} = \mu_0 \mathbf{J} + \mu_0 \varepsilon_0 \frac{\partial \mathbf{E}}{\partial t}.

The last term was Maxwell's own addition. With it, a changing electric field makes a magnetic field and a changing magnetic field makes an electric one, so the fields can sustain each other as a wave travelling through empty space. Its speed is 1/μ0ε01/\sqrt{\mu_0\varepsilon_0}, calculated from laboratory measurements of coils and capacitors, and it came out equal to the measured speed of light. "We can scarcely avoid the inference," Maxwell wrote, "that light consists in the transverse undulations of the same medium which is the cause of electric and magnetic phenomena."

Chapter IV

A Closer Look: The Speed of Light From Coils and Capacitors

Maxwell's equations contain two constants that can be measured on a laboratory bench, with no light involved. The permeability μ0\mu_0 sets how strongly a current produces a magnetic field, and so the force between two wires carrying current. The permittivity ε0\varepsilon_0 sets how strongly charges push on each other, and so how much charge a capacitor holds. In modern units:

μ0=4π×10−7 N/A2,ε0=8.854×10−12 F/m.\mu_0 = 4\pi \times 10^{-7} \text{ N/A}^2 , \qquad \varepsilon_0 = 8.854 \times 10^{-12} \text{ F/m} .

The equations predict waves of electric and magnetic field travelling at

v=1μ0ε0=14π×10−7×8.854×10−12≈2.998×108 m/s.v = \frac{1}{\sqrt{\mu_0 \varepsilon_0}} = \frac{1}{\sqrt{4\pi \times 10^{-7} \times 8.854 \times 10^{-12}}} \approx 2.998 \times 10^8 \text{ m/s} .

That is the speed of light. In 1856 Wilhelm Weber and Rudolf Kohlrausch had measured the corresponding ratio of electrical units, by discharging a capacitor through a galvanometer, and found about 3.1×1083.1 \times 10^8 m/s. Hippolyte Fizeau had measured the speed of light in 1849 with a spinning toothed wheel and a mirror about 8.6 km away, and got about 3.1×1083.1 \times 10^8 m/s as well. Maxwell saw that the agreement could not be a coincidence.

Nothing in the experiments on currents and charges involved light, optics or astronomy. Yet the speed of light fell out of them. Light is an electromagnetic wave, and so, Maxwell predicted, there should be others at every wavelength. Hertz found radio waves twenty years later.

The calculation also carries the puzzle that led to relativity. The formula gives one speed, with no mention of who is measuring it or how fast they are moving. Since 1983 the metre has been defined by fixing the speed of light at exactly 299,792,458 m/s.

Chapter V

Waves and the Missing Ether

In 1887–88 Heinrich Hertz made Maxwell's waves with a spark gap and detected them across his lab. Radio was born, and the theory seemed complete.

But the equations contained a puzzle. They give one speed for light, cc. Relative to what? The natural answer was a medium, the luminiferous ether, at rest in absolute space, with light moving at cc relative to it. The Earth moves through the ether at about 30 km/s around the Sun, so light should travel slightly faster in some directions than others. Albert Michelson and Edward Morley built an interferometer sensitive enough to detect the difference. It found almost nothing.

FitzGerald and Hendrik Lorentz proposed that objects moving through the ether shrink along their direction of motion by exactly enough to hide it. The fix worked but explained nothing. The deeper answer, that there is no ether and that cc is the same for everyone, needed a new idea of time. That idea is special relativity, born at the seam between this field and classical mechanics.

Applications

Where it is used

  • Electric power

    Generators, transformers and the grid

    Almost all electricity is made by spinning coils in magnetic fields, and it is moved across continents by transformers that change its voltage. Both are Faraday's induction. The alternating-current grid is electromagnetism at the scale of civilisation.

  • Communications

    Radio, Wi-Fi and every wireless signal

    Little more than a decade after Hertz's experiments, Guglielmo Marconi was sending radio signals across the Atlantic (1901). Every wireless technology since, from broadcasting to mobile phones, GPS and Wi-Fi, uses Maxwell's waves.

  • Medical imaging↗ Biology

    Magnetic resonance imaging

    MRI scanners place the body in a strong magnetic field and use radio pulses to make hydrogen nuclei signal their positions. Gradient fields encode where each signal came from, a technique introduced by Paul Lauterbur in 1973.

    › Sources (1)
    • Lauterbur, P. C. (1973). Image formation by induced local interactions: examples employing nuclear magnetic resonance. Nature 242: 190–191.
  • Structural biology↗ Biology · Molecular Biology

    X-ray crystallography reveals the molecules of life

    X-rays are electromagnetic waves short enough to diffract off the rows of atoms in a crystal. In 1913 William Lawrence Bragg showed how to read the atomic arrangement from the diffraction pattern. The same method revealed the double helix of DNA and the shapes of thousands of proteins.

    › Sources (1)
    • Bragg, W. L. (1913). The diffraction of short electromagnetic waves by a crystal. Proceedings of the Cambridge Philosophical Society 17: 43–57.

Open problems

Where the map runs out

Conjectured, unproven

Magnetic monopoles

No confirmed detection as of 2026.

Every magnet ever found has both a north and a south pole. Cut one in half and you get two smaller magnets. Paul Dirac showed in 1931 that isolated magnetic charges, monopoles, are allowed by quantum theory. If even one exists, electric charge must come in whole-number units, as it does.

Why it is hard

Grand unified theories predict monopoles, but so heavy that they could only have formed in the early universe and would now be extremely rare. Searches in cosmic rays, old rocks and particle colliders have found none (a single 1982 candidate event was never repeated).

What resolving it unlocks

A detection would explain why electric charge is quantised and would be direct evidence for physics at energies far beyond any collider.

› Sources (1)
  • Dirac, P. A. M. (1931). Quantised singularities in the electromagnetic field. Proceedings of the Royal Society A 133: 60–72.

Further reading

  1. Forbes, N. & Mahon, B. (2014). Faraday, Maxwell, and the Electromagnetic Field. Prometheus Books.

    A readable history of the two men and the idea of the field, for general readers.

  2. Griffiths, D. J. (2017). Introduction to Electrodynamics (4th ed.). Cambridge University Press.

    The standard undergraduate textbook, famously clear.

  3. Feynman, R. P., Leighton, R. B. & Sands, M. (1964). The Feynman Lectures on Physics, Vol. II. Addison-Wesley.

    Electromagnetism from the field outward. Free online.