← Big Ideas of Physics
An interactive field guide

The big ideas of physics

Physics looks for the few rules that everything obeys, from falling apples to distant galaxies and the insides of atoms. Here are twelve of its biggest ideas. Each one comes with a simulation you can run in your browser.

Newton's cannon: fire fast enough and the ball keeps falling around the Earth. That is an orbit.
Part I

Motion

Newton's achievement was to show that one set of rules governs motion everywhere, on Earth and in the heavens. Four ideas carry most of the weight: forces, energy, momentum and gravity.

01

Newton's laws

An object keeps moving at constant speed in a straight line unless a force acts on it. A force changes its velocity in proportion to the force and inversely to its mass.

Aristotle thought motion needed a constant push: stop pushing a cart and it stops. Galileo saw that the cart stops because of friction. Remove friction and a moving object keeps going forever. This is inertia, Newton's first law.

The second law says what a force does: it causes acceleration, a change in velocity. A thrown ball has one force on it in flight, gravity, pulling straight down. So its horizontal speed stays constant while its vertical speed changes steadily, and the result is a parabola. Air resistance adds a second force, opposite to the motion, which shortens the flight and changes the best launch angle.

The third law says forces come in pairs. When you push on a wall, the wall pushes back on you equally hard. That's how rockets work: they push gas backward, and the gas pushes the rocket forward.

F = ma Force = mass × acceleration

History

Galileo rolled balls down ramps in the early 1600s and found that distance grows with the square of time. Newton set out his three laws in the Principia (1687), together with the calculus needed to use them.

Watch out

Heavy objects don't fall faster than light ones. Without air, a hammer and a feather land together, as Apollo 15 astronaut David Scott showed on the Moon in 1971. A feather falls slowly on Earth because of air resistance, not because it's light.

Try it · Launch a projectile
Latest shot Earlier shots
Range — Peak height — Flight time —
Without air, 45° gives the longest range, and angles that add up to 90° (like 30° and 60°) land at the same spot. Try it, then turn on air resistance.
02

Conservation of energy

Energy is never created or destroyed. It only changes form, from motion to height to heat and back.

A swinging pendulum trades two kinds of energy. At the top of its swing it's momentarily still but high up: all potential energy. At the bottom it's low but fast: all kinetic energy. Without friction the total never changes, so it swings back to exactly the same height forever.

Real pendulums slow down, and for a long time that looked like energy being lost. James Joule showed it isn't. Friction turns the energy of motion into heat, in a precise ratio. Count heat as energy and the total is conserved again, in every experiment ever done.

Conservation of energy is a powerful shortcut. You can work out how fast a roller coaster goes at the bottom of a drop from its height alone, without tracking every bump along the way.

½mv² + mgh + heat = constant Kinetic + potential + thermal energy

History

Julius Robert Mayer (1842) and James Joule (1843–1850) established that heat is a form of energy, and Hermann von Helmholtz stated the general law in 1847. In 1918 Emmy Noether proved that energy conservation follows from a deeper fact: the laws of physics are the same today as tomorrow.

Watch out

"Saving energy" in everyday speech really means avoiding turning useful forms (electricity, fuel) into heat we can't use. The energy itself never disappears. What gets used up is its usefulness, which is idea 8.

Try it · Swing a pendulum
Kinetic Potential Heat
The three bars always add up to the same height, even as friction slowly turns the swing into heat.
03

Momentum

Mass times velocity, added up over everything involved, stays the same in every collision, whether the objects bounce apart or stick together.

A heavy truck and a light car moving at the same speed are hard to stop by different amounts. Momentum, mass times velocity, captures that. When two objects collide, they push on each other with equal and opposite forces for the same time (Newton's third law), so whatever momentum one gains, the other loses. The total is conserved.

Energy is a different story. In a perfectly elastic collision, like billiard balls, kinetic energy is conserved too. In an inelastic collision, like two cars crumpling together, some kinetic energy turns into heat, sound and bent metal. Momentum is conserved either way, which is why accident investigators can work backward from where the wreckage ended up.

m₁v₁ + m₂v₂ = m₁v₁′ + m₂v₂′ Total momentum before = total momentum after

History

Descartes made a first attempt at a conservation law for collisions in 1644, but he ignored direction and got it wrong. Christiaan Huygens, John Wallis and Christopher Wren gave correct rules for collisions to the Royal Society in 1668–69.

Watch out

Momentum has a direction. Two equal cars hitting head-on at equal speeds have zero total momentum, so if they stick together they stop dead, even though plenty of energy was involved.

Try it · Collide two carts
04

Universal gravitation

Every mass attracts every other mass. The same force makes things fall and keeps the planets in orbit.

Newton asked whether the force pulling an apple down might reach as far as the Moon. He imagined a cannon on a very tall mountain. A slow cannonball falls to the ground nearby. A faster one lands further away. Fast enough, and the ground curves away beneath it as fast as it falls, so it never lands: it's in orbit. Faster still, and it escapes Earth entirely.

The force falls off with the square of distance. Twice as far away, it's a quarter as strong. That one rule explains the Moon's orbit, the tides, Kepler's laws of planetary motion, and the paths of comets.

F = G m₁m₂r² Low Earth orbit needs about 7.9 km/s, and escape about 11.2 km/s

History

Newton published the law of gravitation in the Principia (1687). Henry Cavendish measured the gravitational constant G in 1798 with a torsion balance, which let him "weigh the Earth." Edmond Halley used Newton's theory to predict the return of his comet in 1758, which it did.

Watch out

Astronauts on the International Space Station aren't weightless because gravity is absent. At their height it's still about 90% as strong as on the ground. They float because they and the station are falling around the Earth together.

Try it · Newton's cannon
Result —
Speeds are scaled to real Earth values from a mountain about 600 km high. Around 7.6 km/s the ball circles the Earth. Above about 10.7 km/s it never comes back.
Part II

Waves and fields

Sound, light and ripples on water are all waves: patterns that travel while the material stays put. Electric and magnetic fields fill space and carry forces and energy, and light turns out to be a wave in those fields.

05

Waves & interference

When two waves overlap, they add. Crest on crest makes a bigger wave, and crest on trough cancels.

Drop two pebbles into a pond and the rings spread through each other. Where crests meet crests the water rises twice as high. Where a crest meets a trough the water stays flat. The result is a fixed pattern of strong and calm lines called interference.

Whether two waves add or cancel at a point depends on the difference in distance to the two sources. A difference of a whole number of wavelengths means they arrive in step and add. A difference of half a wavelength means they cancel. The spacing of the pattern therefore reveals the wavelength, even when it's far too small to see.

Noise-cancelling headphones use the same effect. They play sound that is an exact inverse copy of the noise, so the two cancel at your ear.

bright where path difference = 0, λ, 2λ, …    dark where it's ½λ, 1½λ, … λ (lambda) is the wavelength

History

Thomas Young's double-slit experiment (1801–1803) showed that light makes interference patterns, so light must be a wave. That overturned Newton's view that light was made of particles, until quantum mechanics brought particles back (idea 10).

Watch out

Cancelling waves don't destroy energy. Energy missing from the dark spots shows up in the bright ones, which are brighter than the two waves added separately.

Try it · Two sources in a ripple tank
Light and dark show crests and troughs. The calm lines that fan out between them are where the two waves cancel. Shorter wavelengths or wider separation give more lines.
06

Fields

A charge fills the space around it with an electric field. Other charges feel a force from the field right where they are.

Two charges attract or repel across empty space, with a force that falls off with the square of distance, just like gravity. But how does one charge "know" about the other? Michael Faraday's answer was the field: every charge creates a field that fills the space around it, and other charges respond to the field at their own location.

Fields are real physical things, not just bookkeeping. They carry energy, and changes in them travel at a finite speed. James Clerk Maxwell found that changing electric and magnetic fields keep regenerating each other and travel through space as a wave, at a speed that matched the measured speed of light. Light is an electromagnetic wave. So are radio, microwaves and X-rays.

F = k q₁q₂r² Coulomb's law: like charges repel, opposite charges attract

History

Charles-Augustin de Coulomb measured the force law in 1785. Faraday introduced lines of force in the 1830s and 1840s. Maxwell's equations (1865) unified electricity, magnetism and light, and Heinrich Hertz produced and detected radio waves in 1887.

Watch out

Field lines aren't paths that charges follow. They show the direction of the force at each point. A moving charge can cross field lines, because its momentum carries it.

Try it · Drag the charges
Positive charge Negative charge Field direction (darker = stronger)
Field lines leave positive charges and end on negative ones. Between two like charges there's a point where the fields cancel exactly.
07

Light bends

Light travels more slowly in glass and water than in air. Crossing the boundary at an angle, it changes direction.

A straw in a glass of water looks broken at the surface. That's refraction. Light moves at about 300,000 km/s in a vacuum, but only about 225,000 km/s in water and 200,000 km/s in glass. The ratio is the refractive index n. When a beam enters a slower material at an angle, one side of the beam slows first, and the beam swivels toward the perpendicular, like a marching band stepping onto mud.

Going the other way, from glass into air, the beam bends away from the perpendicular. Beyond a critical angle it can't get out at all, and it reflects completely. Total internal reflection traps light inside optical fibres, which carry most of the world's internet traffic.

n₁ sin θ₁ = n₂ sin θ₂ Snell's law. Lenses, rainbows and fibre optics all follow from it.

History

The law was found by Ibn Sahl in Baghdad around 984, and again by Willebrord Snell in 1621. Pierre de Fermat explained it in 1662 with a principle of least time: light takes the path that gets it there fastest, just as a lifeguard runs further along the beach to swim less.

Watch out

The refractive index varies slightly with colour. Blue light bends a little more than red, which is why prisms and raindrops split white light into a spectrum.

Try it · Aim a laser at a boundary
Refracted angle Critical angle
Part III

Heat and disorder

Energy is conserved, yet some processes only ever run one way. The explanation is statistical: there are overwhelmingly more disordered arrangements than ordered ones.

08

Entropy & the second law

Isolated systems drift toward their most probable state. That makes time's arrow a matter of overwhelming odds.

Open a bottle of perfume and the scent spreads through the room. It never gathers itself back into the bottle. Nothing in the laws of motion forbids that: each molecule's path could run backward just as well. It's just fantastically improbable.

Count the ways. With 100 molecules, there is exactly one arrangement with all of them in the left half of a box, and about 10²⁹ arrangements with 50 in each half. Molecules bounce around at random, so the gas almost always ends up in the kind of state that has the most arrangements. Entropy measures that number of arrangements. The second law of thermodynamics says the entropy of an isolated system practically never decreases.

This is why heat flows from hot to cold, why engines can't turn all their heat into work, and why the past (low entropy) looks different from the future.

S = k log W Boltzmann's entropy: W is the number of microscopic arrangements

History

Sadi Carnot worked out the limits on heat engines in 1824. Rudolf Clausius coined the word "entropy" in 1865. Ludwig Boltzmann explained it statistically in 1877, and S = k log W is carved on his tombstone in Vienna.

Watch out

Entropy can decrease locally. A fridge cools its inside and living things build ordered structures, but only by increasing entropy somewhere else by more, as heat released into the room.

Try it · Remove the partition
On the left now Chance of all being on the left
With 4 particles you'll often see them all return to the left. With 100, never: the chance is 1 in 2¹⁰⁰.
Part IV

Modern physics

Around 1900, experiments at very high speeds and very small scales broke classical physics. Relativity and quantum mechanics replaced it, and both have passed every test since.

09

Relativity

The speed of light is the same for every observer. Keeping it the same forces time itself to run slower for moving clocks.

Einstein started from two assumptions: the laws of physics are the same for everyone moving steadily, and light always travels at the same speed c, however fast you're moving. Those sound harmless, but together they mean time can't be the same for everyone.

Picture a light clock: a pulse bouncing between two mirrors. On a moving train, someone on the platform sees the pulse travel a longer, diagonal path. Light has the same speed for both observers, so each tick must take longer as seen from the platform. Moving clocks run slow by the factor γ (gamma), which is nearly 1 at everyday speeds and grows without limit as speed approaches c.

γ = 1√(1 − v²/c²) At 87% of light speed, γ = 2: a moving clock ticks at half speed

History

Einstein published special relativity in 1905, and E = mc² followed the same year. In 1941 Bruno Rossi and David Hall showed that fast cosmic-ray muons live several times longer than muons at rest, as relativity predicts. GPS satellites would drift by about 38 microseconds a day, about 11 km of position error, without relativistic corrections.

Watch out

Relativity doesn't say "everything is relative." It's built around what's the same for everyone: the speed of light, and the spacetime interval between events. Observers disagree about time and length separately, but agree about how they combine.

Try it · A moving light clock
γ Traveller ages
10

Wave–particle duality

Light and matter arrive in single, particle-like lumps, but where they land is governed by a wave.

Fire electrons, one at a time, at a barrier with two slits. Each electron makes a single dot on the screen, like a particle. But after thousands of dots, a striped interference pattern appears, like the waves of idea 5. Each electron seems to go through both slits and interfere with itself.

Quantum mechanics describes each electron by a wave function. The wave goes through both slits and interferes. Where it's strong, the electron is likely to be found. Where it cancels, the electron never lands. The theory predicts probabilities, not individual outcomes.

Try to find out which slit each electron goes through and the stripes disappear. Gaining that information disturbs the wave, and you get two plain bands instead.

λ = hp De Broglie wavelength: every particle with momentum p has a wavelength

History

Einstein explained the photoelectric effect with particles of light in 1905. Louis de Broglie proposed that matter has waves too (1924), and Davisson and Germer saw electrons diffract off a crystal in 1927. Akira Tonomura's team filmed single electrons building up a two-slit pattern in 1989.

Watch out

"Observing" doesn't require a conscious observer. Any interaction that records which slit the electron took, with a detector, a stray photon or an air molecule, is enough to destroy the pattern.

Try it · One electron at a time
Electrons 0
11

Quantized energy

An electron in an atom can only have certain energies. Jumping between them emits light of exactly one colour, so every element has a fingerprint.

Heat hydrogen gas and pass its glow through a prism. Instead of a rainbow you see a few sharp lines: red, blue-green, and violet. Every element produces its own pattern, and that's how we know what distant stars are made of.

The explanation is that the electron's energy is quantized. In hydrogen it can only have energies of −13.6/n² electronvolts, for n = 1, 2, 3, … When the electron drops from one level to a lower one, it releases the difference as a single photon. A photon's energy fixes its colour, so each possible drop gives one sharp line.

En = −13.6 eVn²    photon energy = Eupper − Elower = hcλ

History

Johann Balmer found a formula for hydrogen's visible lines in 1885 without knowing why it worked. Niels Bohr explained it in 1913 with quantized orbits, and Schrödinger's equation (1926) derived the energy levels from wave mechanics.

Watch out

Electrons don't orbit the nucleus like tiny planets. Bohr's orbits were a stepping stone. In quantum mechanics each level is a cloud-like standing wave with a definite energy but no definite path.

Try it · Make hydrogen glow

Click an upper level, then a lower one, to make the electron jump down and emit a photon.

Jump — Photon energy — Wavelength —
Jumps that end on level 2 give hydrogen's visible lines (the Balmer series). Jumps to level 1 are ultraviolet.
12

Radioactive decay

No one can predict when a single nucleus will decay. But in any large sample, half of them decay in a fixed time, over and over.

An unstable nucleus has a fixed chance of decaying in each second, regardless of its age or what happened before. It has no memory. That one rule produces exponential decay: in each half-life, half of the remaining nuclei decay. After two half-lives a quarter remain, after three an eighth.

Half-lives range from fractions of a second to billions of years, and they're very stable, so radioactive decay works as a clock. Carbon-14, with a half-life of about 5,700 years, dates once-living material up to around 50,000 years old. Uranium–lead dating measures the age of the Earth: about 4.5 billion years.

N(t) = N₀ × (½)t/T T is the half-life

History

Henri Becquerel discovered radioactivity in 1896, and Marie and Pierre Curie isolated polonium and radium in 1898. Ernest Rutherford and Frederick Soddy showed in 1902 that radioactivity transforms one element into another. Willard Libby developed radiocarbon dating in the late 1940s.

Watch out

A half-life isn't a lifespan. A nucleus that has survived ten half-lives is exactly as likely to decay in the next one as a fresh one. And with only a few nuclei, the count jumps around a lot. The smooth curve only emerges in large numbers.

Try it · Watch nuclei decay
Not yet decayed Decayed N₀ × (½)^(t/T)
Half-lives passed 0 Remaining Prediction
Putting it together

Three threads run through all twelve ideas

Conservation laws

Energy, momentum and charge (ideas 2, 3, 6) are never created or destroyed. Noether showed that each conservation law comes from a symmetry: the laws of physics don't change over time, from place to place, or under certain transformations.

Unification

Falling apples and orbiting moons (idea 4), electricity, magnetism and light (ideas 6, 7), heat and molecular motion (idea 8): physics keeps discovering that apparently different phenomena are one thing.

Probability at the root

Entropy, quantum interference, atomic spectra and decay (ideas 8, 10–12) show that the deepest laws are statistical, yet they produce the most precise predictions in science.

Further reading

  • Richard Feynman, The Feynman Lectures on Physics (1963–65; free online). The most famous physics course ever given.
  • Richard Feynman, The Character of Physical Law (1965). Seven lectures on how physics works, for a general audience.
  • Carlo Rovelli, Seven Brief Lessons on Physics (2014). Relativity, quanta and time in under 100 pages.
  • Paul Hewitt, Conceptual Physics. Physics without heavy maths, built around everyday examples.
  • Sean Carroll, From Eternity to Here (2010). Entropy and the arrow of time.
  • PhET Interactive Simulations (University of Colorado Boulder). Hundreds of free physics simulations.