How to read this book
Physics isn't a pile of formulas to memorize — it's humanity's running detective story about how reality behaves. Every equation here was once a mystery that a real, stubborn, often eccentric person cracked. So each idea comes in layers, and you decide how deep to dig.
Use the Essentials / Curious / Deep dive switch at the top. Essentials shows just the headline idea and formula. Curious adds the human story and the real-world uses. Deep dive opens the full step-by-step derivation too. You can also open any single panel by clicking it, or search for a topic.
Motion
The Equations of Motion
For thousands of years, "common sense" said heavier things fall faster and that a moving object naturally slows to a stop. Both are wrong. The first person to replace opinion with measurement — rolling balls down ramps and timing them with his own pulse — kicked off all of modern science. These three little equations are the result.
First equation · \(v = u + at\)
If something speeds up steadily, its final speed is just the start speed plus "how hard it accelerated" times "for how long."
📜 The story ›
Galileo Galilei · Italy · early 1600s
There were no stopwatches. So Galileo slowed motion down by rolling bronze balls down a gently tilted groove, timing them by weighing the water that drained from a vessel during the roll. He discovered that the speed grew in equal steps with equal times — the very definition of constant acceleration. The Church put him under house arrest for unrelated reasons, but this quiet ramp experiment had already cracked the universe open.
✏️ The derivation ›
Acceleration means how much velocity changes each second — the change divided by the time:
Multiply both sides by \(t\):
Add \(u\) to both sides:
🌍 In the real world ›
- Your car's 0–60 time. A "0–60 mph in 5 seconds" rating is exactly this equation in disguise.
- Anti-lock brakes & airbags. A car's safety computer predicts your speed milliseconds ahead using \(v=u+at\) to decide when to fire.
- Rockets and lifts. Engineers cap acceleration so humans aren't crushed — this sets how long the burn must last.
Second equation · \(s = ut + \tfrac12 at^2\)
The distance covered is the steady part \((ut)\) plus an extra bit that grows with the square of time as you keep speeding up.
📜 The story ›
Galileo · the "odd-numbers" rule
Galileo noticed something magical on his ramps: in successive equal time-slices a falling ball covers distances in the ratio 1 : 3 : 5 : 7… Add those up and the totals go 1, 4, 9, 16 — perfect squares. That "distance grows as time squared" is the heartbeat of this formula.
✏️ The derivation ›
With steady acceleration, average velocity is the midpoint of start and end:
Distance = average velocity × time:
Substitute \(v = u+at\):
Split the fraction:
🌍 In the real world ›
- Stopping distances. Why your driving test warns that doubling speed quadruples braking distance — that's the \(t^2\) at work.
- Falling-object safety. Construction nets and crumple zones are sized from how far things fall in a given time.
- Camera-based speed traps. Two photos, a known time gap, and this equation give your speed.
Third equation · \(v^2 = u^2 + 2as\)
A shortcut linking speeds and distance directly — when you don't know (or care about) the time.
✏️ The derivation ›
From the first equation, \(t = \dfrac{v-u}{a}\).
Put it into \(s = \dfrac{u+v}{2}\,t\):
The top is a difference of squares, \((v+u)(v-u)=v^2-u^2\):
Rearrange:
🌍 In the real world ›
- Runway length. Pilots compute the exact tarmac needed to reach take-off speed using this.
- Roller-coaster design. The speed at the bottom of a drop, from the height alone.
- Forensics. Skid-mark length on a road reveals how fast a car was going before braking.
Projectiles & the Art of the Throw
Galileo's second great insight: a thrown object is doing two things at once — coasting sideways at a steady speed while gravity pulls it down. Split them apart, solve each separately, and the graceful curving arc of every basketball, cannonball, and water fountain becomes simple arithmetic.
Time of flight · \(T = \dfrac{2u\sin\theta}{g}\)
How long it hangs in the air depends only on the upward part of the launch.
📜 The story ›
Galileo · and Renaissance gunners
Cannon crews had tables of "how far for which angle," found purely by trial and bloody error. Galileo gave them the why: the curve is a parabola, and horizontal and vertical motion are independent. Drop a bullet and fire one horizontally at the same instant — both hit the ground together. That counter-intuitive fact is the whole chapter.
✏️ The derivation ›
Split the launch: upward part \(u\sin\theta\), sideways part \(u\cos\theta\).
Vertically it returns to the same height, so vertical displacement is zero:
Factor out \(t\) and drop the trivial \(t=0\):
🌍 In the real world ›
- Sports. A goalkeeper's punt, a golfer's loft, a long-jumper's take-off — all tuned for hang time.
- Fireworks. Fuses are timed so shells burst at the top of the arc, where they hang longest.
Maximum height · \(H = \dfrac{u^2\sin^2\theta}{2g}\)
How high it climbs before gravity wins and it starts falling.
✏️ The derivation ›
At the top the upward speed is momentarily zero. Use \(v^2=u_y^2-2gH\) with final speed 0:
Solve for \(H\):
🌍 In the real world ›
- Fountains & sprinklers. Nozzle pressure is set to reach a target height.
- Volleyball & basketball. Players intuitively solve this every time they arc a shot over a defender.
Range · \(R = \dfrac{u^2\sin 2\theta}{g}\)
How far it travels — and the reason 45° throws the farthest.
✏️ The derivation ›
Sideways speed is constant, so range = sideways speed × flight time:
Use the identity \(2\sin\theta\cos\theta=\sin 2\theta\):
🌍 In the real world ›
- Shot put & javelin. Athletes release a touch below 45° because they launch from shoulder height, not the ground.
- Artillery & ballistics. The original reason this maths was funded for centuries.
- Water-jet cutting & irrigation. Reach is optimised with the same rule.
Forces & Energy
Force & Momentum
In 1665 a plague shut the universities, and a 23-year-old went home to the countryside for two years. Alone, Isaac Newton invented calculus, split white light, and worked out the laws of motion and gravity. He later called it his "year of wonders." Almost everything in this chapter was born in that quiet, locked-down farmhouse.
Newton's second law · \(F = ma\)
Push something: the harder you push, the faster it speeds up — and heavier things are stubborner.
📜 The story ›
Isaac Newton · England · 1687, the Principia
Newton didn't actually write "\(F=ma\)." His real law spoke of momentum — the "quantity of motion" — and said force changes it. That deeper version still works when mass changes, like a rocket burning fuel. Newton was secretive, vengeful in feuds, and obsessed with alchemy — yet he gave us the rulebook the universe had been using all along.
✏️ The derivation ›
Newton's true statement: force is the rate of change of momentum \(p=mv\):
If mass is constant, only velocity changes:
And \(\dfrac{\Delta v}{\Delta t}\) is exactly acceleration:
🌍 In the real world ›
- Everything you build. Bridges, cranes, elevators, robot arms — all sized with \(F=ma\).
- Rockets. The momentum form explains thrust: throw mass backwards fast, get pushed forwards.
- Crash safety. Heavier cars need more force to stop — central to vehicle design and ratings.
Impulse · \(F\,t = \Delta p\)
A small force over a long time can change motion as much as a big force over an instant.
✏️ The derivation ›
Start from \(F=\dfrac{\Delta p}{\Delta t}\).
Multiply both sides by the time \(\Delta t\):
🌍 In the real world ›
- Airbags & crumple zones. They stretch out the stopping time, slashing the force on your body.
- Catching an egg. You move your hands back — more time, less force, no mess.
- Boxing & martial arts. "Rolling with a punch" lengthens contact time to soften the blow.
Conservation of momentum · \(\sum p = \text{const}\)
In any collision or explosion, the total "quantity of motion" before equals the total after.
✏️ The derivation ›
By Newton's third law, A pushes B exactly as hard as B pushes A, oppositely: \(F_{AB}=-F_{BA}\).
They're in contact the same time, so their momentum changes are equal and opposite: \(\Delta p_B = -\Delta p_A\).
One gains what the other loses — total change is zero:
🌍 In the real world ›
- Rockets in empty space. With nothing to push against, they throw exhaust one way to go the other. This is how we reach the planets.
- Newton's cradle & billiards. The click-clack of transferred momentum.
- Recoil. Why a fired gun kicks back and a squid jets forward.
Energy & Power
"Energy" feels obvious now, but it took a century of argument to pin down. A brewer's son measuring the warmth of churning water, and a brilliant marquise translating Newton by candlelight, helped prove that energy is never created or destroyed — only passed around in disguise.
Kinetic energy · \(E_k = \tfrac12 mv^2\)
The energy of motion — and notice it depends on speed squared, so going twice as fast carries four times the punch.
📜 The story ›
Émilie du Châtelet · France · 1740s
Most scholars thought "energy of motion" went as \(mv\). Émilie du Châtelet — a French mathematician who dropped weights into clay to measure the dents — showed the dent depth (the real effect) scaled with \(mv^2\), not \(mv\). She was right, and her insight survives in the \(v^2\). She translated Newton into French while pregnant at 42, and finished days before she died.
✏️ The derivation ›
Work done by a force over a distance becomes energy of motion: \(W=Fs\), and \(F=ma\):
Starting from rest, \(v^2=2as\), so \(as=\tfrac12 v^2\):
That stored work is the kinetic energy:
🌍 In the real world ›
- Speed limits save lives. The \(v^2\) is why a crash at 60 is far more than twice as deadly as at 30.
- Wind turbines. Power scales with wind speed cubed — a windy day is gold.
- Hydroelectric dams. Falling water's kinetic energy spins generators.
Potential energy · \(E_p = mgh\)
Energy stored simply by being up high, ready to be released by falling.
✏️ The derivation ›
To lift slowly you push up against gravity with force \(mg\).
Work = force × height lifted:
🌍 In the real world ›
- Pumped-storage power. Grids pump water uphill when power is cheap, release it when demand spikes — the world's biggest "battery."
- Roller coasters. The first big climb stores all the energy the rest of the ride spends.
Power · \(P = Fv\)
Power is how fast you deliver energy — the difference between a sprint and a stroll up the same hill.
✏️ The derivation ›
Power is work per unit time, and work is \(Fs\):
And \(\dfrac{s}{t}\) is the speed \(v\):
🌍 In the real world ›
- "Horsepower." James Watt coined it to sell steam engines by comparing them to horses.
- Your electricity bill. Charged in kilowatt-hours — power multiplied by time.
- Cycling & fitness. Smart trainers report your power output in watts in real time.
Going in Circles
Here's a brain-bender: an object whirling at perfectly steady speed is still accelerating — because its direction keeps changing, and velocity is about direction too. Something must constantly yank it toward the centre, or it flies off in a straight line. That inward pull rules everything from a hammer throw to a satellite.
Centripetal acceleration · \(a = \dfrac{v^2}{r}\)
To keep curving, you need an inward acceleration that grows fiercely with speed and bites harder on tight turns.
📜 The story ›
Christiaan Huygens · Netherlands · 1659
Huygens — the same genius who built the first pendulum clock and spotted Saturn's rings — was first to nail the "centre-seeking" force mathematically. The word centripetal (Latin for "centre-seeking") was later coined by Newton, who used Huygens' result to prove the Moon is simply falling around the Earth.
✏️ The derivation ›
In a short time \(\Delta t\) the object sweeps a small angle \(\Delta\theta = \dfrac{v\,\Delta t}{r}\) around the circle.
The velocity arrow (length \(v\)) swings through that same angle, so it changes by \(\Delta v = v\,\Delta\theta\):
Acceleration is \(\dfrac{\Delta v}{\Delta t}\):
🌍 In the real world ›
- Banked race tracks & highway curves. Tilted so the road itself supplies the inward push.
- Washing machine spin cycle. Water flies outward through the drum holes while clothes are held in.
- Centrifuges. Spin blood or DNA fast enough and heavy bits separate — vital in hospitals and labs.
- Satellites. Gravity is the inward pull keeping them circling instead of flying off.
Gravity & the Heavens
Newton's leap was almost unbelievable: the same force that makes an apple fall holds the Moon in its orbit and steers the planets. One law, written once, governs an apple and a galaxy. It let humans predict eclipses centuries ahead and, eventually, fling spacecraft to other worlds.
Surface gravity · \(g = \dfrac{GM}{R^2}\)
Why everything falls at the same rate — and why that rate depends on the planet, not on you.
📜 The story ›
Newton (1687) & Henry Cavendish (1798)
Newton's law had a mystery number \(G\) nobody could measure. Over a century later, the reclusive Henry Cavendish hung lead balls from a delicate twisting wire in a sealed shed and watched them tug on each other by a hair's breadth. He had, in effect, weighed the Earth — one of the most exquisite experiments ever performed.
✏️ The derivation ›
Newton's gravity on a mass \(m\) at a planet's surface:
That force is the weight, also written \(mg\). Set them equal:
The \(m\) cancels — so every object falls identically:
🌍 In the real world ›
- You'd weigh ~⅓ as much on Mars. Same you, smaller planet, smaller \(g\).
- Oil & mineral hunting. Tiny local changes in \(g\) reveal dense ore or hidden caverns underground.
Orbital & escape velocity · \(v_e = \sqrt{\dfrac{2GM}{R}}\)
There's a precise speed to circle a planet, and a faster one to leave it forever.
✏️ The derivation ›
Orbit: gravity supplies the centripetal force, so \(\dfrac{GMm}{r^2}=\dfrac{mv^2}{r}\). Cancel and solve:
Escape: to just break free, kinetic energy must cancel gravitational energy (total energy zero):
Cancel \(m\), times 2, square root:
🌍 In the real world ›
- Every rocket launch. Mission planners must hit orbital speed (~7.8 km/s) precisely, or escape speed to reach other planets.
- GPS & communications satellites. Parked at the exact radius where orbital period equals one day, so they hover over the same spot.
- Black holes. A black hole is just a place where escape velocity exceeds the speed of light — so not even light gets out.
Kepler's third law · \(T^2 \propto r^3\)
Distant planets don't just travel farther — they also crawl slower, in a precise mathematical lockstep.
📜 The story ›
Johannes Kepler · 1619 · from Tycho Brahe's data
Kepler inherited decades of obsessively precise naked-eye observations from the flamboyant Danish astronomer Tycho Brahe (who had a metal nose after a duel). After years wrestling with the numbers, Kepler found the planets trace ellipses, not perfect circles — and that this clean \(T^2\propto r^3\) ratio held for every one. Newton later proved it falls straight out of gravity.
✏️ The derivation ›
Period = circumference ÷ orbital speed, with \(v=\sqrt{GM/r}\):
Tidy: \(\dfrac{r}{\sqrt{1/r}}=r^{3/2}\), then square both sides:
🌍 In the real world ›
- Weighing distant stars. Watch a planet's period and distance, and this equation hands you the star's mass.
- Hunting exoplanets. Astronomers use it to map alien solar systems light-years away.
Spin & Rotation
Straight-line rules have twirling twins. Push becomes twist (torque), mass becomes "how spread out" (moment of inertia), and momentum becomes angular momentum — the quantity a spinning skater hoards to whirl faster. Once you see the parallel, half of rotation is free.
Newton's law for spinning · \(\tau = I\alpha\)
Twist (torque) makes things spin up, but fat, spread-out objects resist — that's their moment of inertia.
📜 The story ›
Leonhard Euler · 1700s
Newton gave us straight-line motion; the staggeringly prolific Swiss mathematician Leonhard Euler built the rotational version. Even after going blind, Euler kept producing maths at a furious pace, dictating to assistants — including the equations that let us spin everything from flywheels to spacecraft on purpose.
✏️ The derivation ›
Take a single mass \(m\) on a spoke of radius \(r\). A tangential force gives it \(F=ma\), and its line-speed acceleration relates to spin via \(a=r\alpha\):
Torque is "force × lever arm," \(\tau=Fr\). Multiply through by \(r\):
The combination \(mr^2\) is the moment of inertia \(I\) — rotational "stubbornness":
🌍 In the real world ›
- Why door handles are far from the hinge. More lever arm = more torque for the same push.
- Wrenches & engines. Your car's "torque" rating is its twisting muscle; a longer wrench loosens stubborn bolts.
- Tightrope walkers' long poles. They add moment of inertia, making tipping slow and correctable.
Conservation of angular momentum · \(L = I\omega = \text{const}\)
Pull your spinning mass inward and you must spin faster — the secret behind every figure-skating finale.
✏️ The derivation ›
With no outside twist, angular momentum \(L=I\omega\) can't change.
A skater pulling her arms in shrinks \(I\) (mass moves closer to the axis). For \(L\) to stay fixed, \(\omega\) must rise:
🌍 In the real world ›
- Figure skaters & divers. Arms in to spin up, arms out to slow down — live physics on ice.
- Helicopters' tail rotors. They exist purely to counter the body's tendency to spin the opposite way.
- Neutron stars. A dying star collapses to city size and spins up to hundreds of times per second.
- How a falling cat lands on its feet. It twists one half against the other while conserving \(L\).
Fluids & Flight
Liquids and gases can't be pushed like solid blocks, yet they obey beautifully simple rules. Two ancient and not-so-ancient discoveries — one shouted from a bathtub, one that keeps 400-tonne jets in the sky — show how pressure does the heavy lifting.
Archimedes' principle · \(F_{\text{buoy}} = \rho g V\)
Anything in a fluid is pushed up by the weight of the fluid it shoves out of the way.
📜 The story ›
Archimedes · Syracuse · ~250 BCE
A king suspected his gold crown was secretly cut with cheap silver. Archimedes, stepping into a full bath and watching it overflow, realised submerged objects displace their own volume — and reportedly ran naked through the streets yelling "Eureka!" ("I've found it!"). By comparing the crown's displacement to pure gold, he could expose the fraud without melting a thing.
✏️ The derivation ›
Fluid pressure grows with depth: \(P=\rho g h\). So the bottom of a submerged block feels more pressure than its top.
For a block of area \(A\) and height \(H\), the net upward push is the pressure difference times area:
But \(H\cdot A\) is just the block's volume \(V\):
🌍 In the real world ›
- Why steel ships float. Hollow hulls displace enormous volumes of water — the upward push beats their weight.
- Submarines. Flood or empty tanks to tune buoyancy and dive or surface.
- Hot-air balloons. Same idea in air: warm, light air displaces cooler, heavier air.
Bernoulli's principle · \(P + \tfrac12\rho v^2 + \rho g h = \text{const}\)
Speed a fluid up and its pressure drops — the quiet trick behind wings, sails, and spinning footballs.
📜 The story ›
Daniel Bernoulli · Switzerland · 1738
Daniel Bernoulli came from a family of mathematicians so competitive that his own father reportedly tried to steal credit for his work and barred him from home. Undeterred, Daniel realised a fluid's energy is shared between pressure, motion, and height — and that the three trade off. Speed rises, pressure falls.
✏️ The derivation ›
It's energy conservation for a flowing parcel of fluid. Each unit of volume carries three energy "currencies": pressure energy \(P\), motion energy \(\tfrac12\rho v^2\), and height energy \(\rho g h\).
With no friction, the total can't change as the fluid flows along:
🌍 In the real world ›
- How planes fly. Air rushes faster over the curved top of a wing, lowering pressure there and lifting the plane (it works together with the wing deflecting air downward).
- Curveballs & "bending it like Beckham." Spin makes one side of the ball move faster through the air, bending its path.
- Carburettors, perfume atomisers, chimney draughts. Fast-moving air sucks fluid along with it.
Vibrations & Waves
Swings & Springs
Anything that gets pulled back harder the further it strays — a pendulum, a guitar string, an atom in a crystal — wobbles in the same elegant rhythm called simple harmonic motion. Master one spring and you've understood a stunning slice of the universe.
Mass on a spring · \(T = 2\pi\sqrt{\dfrac{m}{k}}\)
Heavier masses bob slowly; stiffer springs snap back fast. The period captures both.
📜 The story ›
Robert Hooke · England · 1660
Hooke — Newton's brilliant, prickly rival — found that a spring's pull is simply proportional to its stretch. He first published it as a scrambled Latin anagram (ceiiinosssttuv) to claim priority while keeping it secret, later revealing "ut tensio, sic vis" — "as the stretch, so the force." Pure scientific drama.
✏️ The derivation ›
Hooke's law gives the restoring force \(F=-kx\). With \(F=ma\):
Harmonic motion always has the form \(a=-\omega^2 x\). Matching gives \(\omega^2=\dfrac{k}{m}\), and the period is \(T=\dfrac{2\pi}{\omega}\):
🌍 In the real world ›
- Car suspension. Springs and dampers tuned so you glide, not bounce, over bumps.
- Skyscrapers in earthquakes. Giant "tuned mass dampers" sway to cancel the building's wobble.
- Quartz watches. A tiny vibrating crystal keeps time to within seconds a month.
The simple pendulum · \(T = 2\pi\sqrt{\dfrac{L}{g}}\)
A pendulum's swing depends only on its length and gravity — not on how heavy the bob is, nor (for small swings) how far it swings.
📜 The story ›
Galileo · bored in church, ~1583
Legend says a teenage Galileo, watching a lamp swing in Pisa cathedral, timed it against his own pulse and noticed each swing took the same time regardless of size. That observation became the pendulum clock and ruled timekeeping for 300 years — accurate navigation at sea once depended on it.
✏️ The derivation ›
The restoring pull is gravity's sideways component, \(F=-mg\sin\theta\). For small angles, \(\sin\theta\approx\theta\):
Along the arc, displacement \(x=L\theta\), so \(\theta=x/L\):
This is \(F=-kx\) with \(k=\dfrac{mg}{L}\). Drop it into the spring result; the mass cancels:
🌍 In the real world ›
- Grandfather clocks. A roughly 1-metre pendulum ticks once a second — by design.
- Measuring gravity. Time a pendulum and you can measure \(g\), and so map what's buried below.
- Metronomes & playground swings. Same rhythm, same equation.
Waves & Sound
A wave is a clever trick: energy travels across a room while the stuff it travels through — air, water, a rope — mostly just jiggles in place. The same rules describe ripples on a pond, the note of a violin, light from a star, and the wifi reaching this page.
The wave equation · \(v = f\lambda\)
A wave's speed is just how many wavelengths pass each second, each a wavelength long.
✏️ The derivation ›
In one full cycle the wave advances exactly one wavelength \(\lambda\), taking one period \(T\). Speed = distance ÷ time:
Frequency is cycles per second, \(f=1/T\):
🌍 In the real world ›
- Radio & wifi. Stations are labelled by frequency (e.g. 98.5 FM); this equation converts that to wavelength for antenna design.
- Musical instruments. Shorter strings/pipes → higher frequency → higher pitch.
- Microwave ovens. A fixed wavelength creates hot/cold spots — which is why the plate rotates.
The Doppler effect · \(f' = f\left(\dfrac{v}{v - v_s}\right)\)
An approaching source bunches its waves up, raising the pitch; as it passes and recedes, the pitch drops — the "neeee-yowww" of a passing car.
📜 The story ›
Christian Doppler · 1842 · tested with trumpeters on a train
Doppler predicted moving sources should shift in pitch. To test it, a Dutch scientist hired a brass band to play a steady note aboard an open railway carriage while listeners on the platform noted the change. The pitch dropped as it passed — exactly as predicted. A brass band on a moving train confirmed a law now used to scan unborn babies and measure the expanding universe.
✏️ The derivation ›
In one period the source emits a wave but also creeps forward \(v_s T\), squashing the wavelength ahead:
The sound still travels at \(v\), so the heard frequency \(f'=v/\lambda'\). Using \(\lambda=vT\) and \(1/T=f\):
🌍 In the real world ›
- Doppler ultrasound. Measures blood flow and a baby's heartbeat from how sound bounces off moving cells.
- Police & weather radar. Speed guns and storm tracking both read the frequency shift.
- The expanding universe. Light from distant galaxies is shifted toward red — the cosmic Doppler effect that revealed the Big Bang.
Heat & Matter
Heat & the Restless Atom
For ages, heat was imagined as a mysterious invisible fluid called "caloric." The truth is wilder and simpler: heat is just jiggling. Temperature is the average speed of countless atoms zooming and bouncing. Pressure is their constant drumming on the walls. This insight unified heat with motion — and proving atoms were real cost one of its champions his life.
Pressure of a gas · \(P = \tfrac13\rho\,\overline{v^2}\)
The push of a gas is nothing but the combined hammering of trillions of tiny molecules against the container.
📜 The story ›
Maxwell, Boltzmann & the reality of atoms · late 1800s
James Clerk Maxwell and Ludwig Boltzmann built the picture of gases as swarms of bouncing molecules. Many leading scientists still didn't believe atoms even existed, and Boltzmann was attacked relentlessly for insisting they did. Battling depression and ridicule, he died by suicide in 1906 — just as the tide turned. His tombstone is engraved with his entropy equation. He was right; atoms are real.
✏️ The derivation ›
One molecule (mass \(m\)) hits a wall and rebounds, reversing its momentum by \(2mv_x\).
In a box of side \(L\) it comes back every \(\dfrac{2L}{v_x}\) seconds, so the force it exerts is:
For \(N\) molecules, pressure = total force ÷ wall area, with volume \(V=L^3\):
Motion is random in 3 directions so \(\overline{v_x^2}=\tfrac13\overline{v^2}\), and \(\rho=Nm/V\):
🌍 In the real world ›
- Why a hot tyre reads higher pressure. Hotter air = faster molecules = harder drumming.
- Pressure cookers & engines. Heating trapped gas raises pressure to cook fast or drive pistons.
- Weather. Warm air's extra molecular bounce drives winds, storms, and pressure systems.
The Laws of Heat
Thermodynamics began with a very practical question — how to get more work out of a steam engine — and ended up explaining why time only runs forwards, why perpetual-motion machines are impossible, and perhaps how the universe will end. Few fields travel so far from such humble origins.
First law · \(\Delta U = Q - W\)
Energy is never free: the heat you add either warms a thing up or gets spent doing work. Books always balance.
📜 The story ›
James Joule · England · 1840s
Joule, a brewer by trade, obsessively measured how stirring, friction, and electricity all turned into the same amount of heat. He even tried to measure the warming of waterfalls on his honeymoon. His painstaking work proved heat and work are two faces of one thing — energy — which is why the unit of energy bears his name.
✏️ The derivation ›
This is conservation of energy applied to heat. A system's internal energy \(U\) (its stored molecular jiggling) can change two ways:
You can pour heat \(Q\) in, or the system can spend energy doing work \(W\) out. The net change is the difference:
🌍 In the real world ›
- Engines & power plants. Every one is heat in, work out, accounted to the joule.
- Refrigerators & air conditioners. Run the law backwards: do work to pump heat from cold to hot.
- Your body. Food energy in = work done + heat radiated. Dieting is thermodynamics.
The second law & entropy · \(\Delta S \ge 0\)
Left alone, things get messier, heat flows from hot to cold, and you can never turn heat fully back into work. Disorder always wins.
📜 The story ›
Sadi Carnot (1824) & Rudolf Clausius (1865)
A young French engineer, Sadi Carnot, asked the best possible efficiency of a steam engine — and discovered a hard ceiling no machine can beat. Clausius later named the quantity that always grows: entropy. It's the deepest "you can't win, and you can't break even" rule in all of science, and it gives time its one-way arrow.
✏️ The derivation ›
Entropy measures how many microscopic arrangements look the same from outside — roughly, "how disordered." A shuffled deck has vastly more arrangements than a sorted one.
Because disordered states are overwhelmingly more numerous, random jostling almost always lands you in one. So for any isolated system:
🌍 In the real world ›
- Why your coffee always cools. Heat flows to the cold room, never spontaneously back.
- Engine efficiency limits. Even a perfect car engine wastes most of its fuel as heat — by law, not by sloppiness.
- The arrow of time. The past differs from the future only because entropy was lower back then. It may even decide the fate of the cosmos.
Electricity & Magnetism
Electric Currents
Tame the flow of invisible electrons and you can light a city. The rules turn out to be reassuringly like water in pipes: voltage is the pressure, current is the flow, resistance is the narrowness. From that plumbing analogy, the whole electric world unfolds.
Resistors in series · \(R = R_1 + R_2\)
Line resistors up one after another and their resistances simply add — like adding pipe length.
📜 The story ›
Georg Ohm · Germany · 1827
Ohm published his neat law relating voltage, current, and resistance — and was met with scorn. Critics called it "a web of naked fantasies"; he resigned his teaching post in disgrace. Decades later he was vindicated and honoured, and the unit of resistance now carries his name. Being right early is often lonely.
✏️ The derivation ›
In series the same current \(I\) flows through both, and their voltage drops add: \(V=V_1+V_2\).
Apply Ohm's law \(V=IR\) to each:
Divide by the common \(I\):
🌍 In the real world ›
- Old fairy lights. One bulb dies and the whole string goes dark — classic series wiring.
- Dimmers & volume knobs. Add resistance in line to throttle current.
Resistors in parallel · \(\tfrac1R = \tfrac1{R_1}+\tfrac1{R_2}\)
Side-by-side paths give the current more room, so the combined resistance is lower than either alone.
✏️ The derivation ›
In parallel both feel the same voltage \(V\), and the current splits: \(I=I_1+I_2\).
Use \(I=V/R\) for each branch:
Divide through by \(V\):
🌍 In the real world ›
- Your home wiring. Every socket is in parallel, so each gets the full 230 V (or 120 V) and one switch-off doesn't kill the rest.
- The power grid. Adding users in parallel keeps everyone's voltage steady.
Energy in a capacitor · \(E = \tfrac12 CV^2\)
Capacitors store charge like a coiled spring stores push — ready to dump energy in a flash.
✏️ The derivation ›
As you charge it, the voltage rises with the charge already on it: \(V=q/C\). Adding a sliver \(\mathrm{d}q\) costs \(\dfrac{q}{C}\mathrm{d}q\).
Sum it up from 0 to \(Q\) (the area under the \(V\)–\(q\) line):
Using \(Q=CV\):
🌍 In the real world ›
- Camera flash. A capacitor charges slowly, then dumps it all in a blinding millisecond.
- Defibrillators. Store a controlled jolt of energy to restart a heart.
- Every electronic device. Capacitors smooth power and keep memory alive between blinks.
Magnetism & Induction
The single most important discovery for modern life might be this: move a magnet near a wire and electricity appears, from nothing. That one fact powers every generator on Earth — the dams, the wind farms, the power stations. A self-taught bookbinder's apprentice found it.
Electromagnetic induction · \(\mathcal{E} = BLv\)
Sweep a wire of length \(L\) through a magnetic field at speed \(v\) and you generate a voltage out of pure motion.
📜 The story ›
Michael Faraday · England · 1831
Faraday left school at 13 and taught himself science while binding books. With almost no maths, his sheer experimental genius revealed that a changing magnetic field creates electricity. Asked by a politician what use it could possibly be, he reportedly replied, "One day, sir, you may tax it." He was right — induction now generates virtually all the world's power.
✏️ The derivation ›
A magnetic field pushes on moving charges with force \(F=qvB\). Drag a wire through the field and its free electrons feel this push along the wire.
That push acts like a battery. The "voltage" (EMF) is force-per-charge times the wire length \(L\):
So motion through a field literally manufactures voltage:
🌍 In the real world ›
- Every power station. Coal, nuclear, hydro, wind — all just spin magnets near coils to induce current. The fuel only turns the turbine.
- Electric motors. Run induction backwards: feed in current near a magnet and get motion. Fans, trains, hard drives, EVs.
- Phone wireless charging & induction stoves. A changing field induces current (or heat) with no wires touching.
- Regenerative braking. An EV slowing down turns its motor into a generator, recapturing energy into the battery.
Light & the Modern World
Light & Optics
Bend light and you can correct a child's eyesight, see a living cell, or photograph a galaxy. The rules of how light turns and focuses are ancient, but understanding why light bends — because it slows down in glass and water — is one of physics' most satisfying "aha"s.
Snell's law · \(n_1\sin\theta_1 = n_2\sin\theta_2\)
Light bends when it changes speed crossing into a new material — the reason a straw looks broken in a glass of water.
📜 The story ›
Ibn Sahl (984), Snellius (1621), and Newton's prism
The Persian scholar Ibn Sahl described the bending of light over 600 years before the Dutchman Willebrord Snell rediscovered it. Then Isaac Newton passed sunlight through a prism and split it into a rainbow, proving white light is a mixture of colours — each bending by a slightly different amount. Optics is a thousand-year relay race.
✏️ The derivation ›
Picture a wide wavefront hitting the surface at a slant. One edge enters the slower medium first and slows, while the other edge races on — so the front pivots, like a marching band wheeling when one flank takes shorter steps.
The geometry gives \(\dfrac{\sin\theta_1}{\sin\theta_2}=\dfrac{v_1}{v_2}\). Refractive index is defined as \(n=c/v\), so \(v=c/n\). Substitute; the \(c\)'s cancel:
Cross-multiply:
🌍 In the real world ›
- Glasses, contacts & cameras. Every lens bends light by this rule to focus an image.
- Rainbows & diamonds. Different colours bend differently, scattering light into spectra and sparkle.
- Fibre-optic internet. Light is trapped inside glass strands by total internal reflection — Snell's law taken to its extreme.
The lens & mirror formula · \(\tfrac1v + \tfrac1u = \tfrac1f\)
A single tidy relation ties where an object sits, where its image forms, and the lens's focusing power.
✏️ The derivation ›
Trace two rays from the object: one through the lens centre (straight through), one parallel to the axis (bent through the focus \(F\)). Where they cross is the image.
This builds two pairs of similar triangles (same shape, different size). One pair links the image and object heights to \(u\) and \(v\); the other links them through \(f\).
Setting the matching ratios equal and cancelling the shared heights gives:
🌍 In the real world ›
- Telescopes & microscopes. Galileo's telescope revealed Jupiter's moons; this formula sizes every one since.
- Your phone camera. Tiny lenses positioned by this equation to focus on near or far.
- Your own eyes. The lens flexes to change \(f\); glasses correct it when it can't focus right.
The Quantum & Relativity
Around 1900, physics seemed nearly finished — and then it shattered, gloriously. Light turned out to come in lumps, matter turned out to ripple like waves, mass turned out to be frozen energy, and time itself turned out to bend with speed. Welcome to the strangest, most powerful ideas humans have ever had.
The photoelectric equation · \(E_k = hf - \phi\)
Light arrives in discrete packets (photons). Each one frees one electron — and only if it carries enough energy.
📜 The story ›
Max Planck (1900) & Albert Einstein (1905)
Planck reluctantly proposed that energy comes in tiny indivisible chunks ("quanta") to fix a stubborn problem — and called it a desperate act. Einstein took it literally: light itself is lumps. In his "miracle year" of 1905, while working as a patent clerk, Einstein explained the photoelectric effect this way. It won him the Nobel Prize — not relativity — and launched quantum physics.
✏️ The derivation ›
Each photon delivers a fixed energy \(hf\) to a single electron — all or nothing.
Some energy \(\phi\) (the "work function") is spent just escaping the metal. By energy conservation, the rest becomes motion:
🌍 In the real world ›
- Solar panels. Photons knock electrons loose to make electricity — the photoelectric effect powering the planet.
- Digital cameras & phone sensors. Each pixel counts photons hitting it.
- Automatic doors & night-vision. Light sensors built on the same physics.
Matter waves · \(\lambda = \dfrac{h}{p}\)
If light can act like particles, then particles — even you — can act like waves. They just have an unimaginably tiny wavelength.
📜 The story ›
Louis de Broglie · France · 1924 (a PhD thesis!)
A French aristocrat proposed in his doctoral thesis that matter has a wavelength. His examiners were so baffled they sent it to Einstein, who declared it brilliant. Within years, electrons were shown to diffract like waves, and de Broglie won the Nobel Prize — for a student dissertation.
✏️ The derivation ›
A photon's momentum is \(p=hf/c=h/\lambda\).
de Broglie's leap: turn it around. Anything with momentum \(p\) must have a wavelength:
🌍 In the real world ›
- Electron microscopes. Electrons' tiny wavelength lets us see viruses and atoms, far beyond light microscopes.
- Modern chemistry. The wave nature of electrons explains the shapes of atoms and every chemical bond.
Mass–energy · \(E = mc^2\)
Mass and energy are the same thing in different clothes — and the exchange rate, \(c^2\), is colossal.
📜 The story ›
Albert Einstein · 1905
Buried in a three-page afterthought to his relativity paper, Einstein asked whether an object's mass depends on its energy content — and answered yes. A speck of matter holds staggering energy. This single line explains why the Sun shines, and, more darkly, the power of the atom.
✏️ The derivation ›
Light carries momentum \(p=E/c\). Imagine a sealed box that emits a flash of light energy \(E\) from one end; like a gun, the box recoils.
For the box's centre of mass to stay put (no outside force allowed), the energy that crossed the box must have carried mass with it. Balancing the momentum books, that mass satisfies:
🌍 In the real world ›
- The Sun & stars. Fusing hydrogen converts a sliver of mass into the sunlight that grows our food.
- Nuclear power. Splitting heavy atoms turns mass-defect into electricity for millions.
- PET scans. Antimatter in hospitals annihilates with matter, turning mass fully into detectable energy.
Time dilation · \(t = \dfrac{t_0}{\sqrt{1 - v^2/c^2}}\)
Move fast and your clock genuinely runs slow compared to someone standing still. Time is not the same for everyone.
📜 The story ›
Albert Einstein · 1905 · special relativity
Einstein started from one stubborn fact: everyone measures light at the same speed, no matter how they move. Following that ruthlessly to its conclusions, he found that time and space themselves must stretch and squeeze. The cost of light's constancy is that simultaneity, duration, and length all become relative.
✏️ The derivation ›
Picture a "light clock": a pulse bouncing straight up and down between two mirrors, ticking once per round trip.
To someone watching it fly past at speed \(v\), the pulse travels a longer diagonal path. But light's speed \(c\) is fixed for everyone — so a longer path must take longer. By Pythagoras on the diagonal:
Solve for the moving time \(t\):
🌍 In the real world ›
- GPS satellites. Their fast-moving, high-altitude clocks drift relative to ours; without relativity corrections, GPS would be off by kilometres within a day.
- Particle accelerators. Short-lived particles live measurably longer when whizzing near light speed — time dilation seen daily.
- Cosmic-ray muons. They reach the ground only because their internal clocks run slow on the way down.
"The most incomprehensible thing about the universe is that it is comprehensible."
— a sentiment often attributed to Einstein
Every formula in this book was once impossible, then mysterious, then obvious. The next ones are still out there, waiting for someone curious enough to ask why. Maybe you.