Physics, drawn.

Physics is taught in equations and understood in pictures, and the pictures are usually the part left out. This is a collection of essays about the second kind — one idea at a time, illustrated to the point where the argument becomes visible.

The field of a dipoleField lines traced from a positive charge toward a negative one. Every line does eventually close on the negative charge, but the outer ones loop far outside any frame, so this picture is a crop rather than the whole field.+
Fig. 1 The field around a positive and a negative charge. Every line is traced by stepping along the local field direction, so the shape is a consequence of the inverse-square law rather than a drawing of what it ought to look like. The lines running off the edge do close on the negative charge — they simply do it outside the frame.

Start anywhere

19 essays

−π−π/2π/2π-22angleangular velocityat rest, hanging downbalanced upside downclosed: swingingopen: going over the topdashed: the boundary Mechanics

The pendulum, and the small lie that makes it simple

A pendulum's period does not depend on how far it swings. This is one of the most useful false statements in physics, and it is worth knowing exactly how false.

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00.20.40.60.8100.20.4range20°35°45°60°75°same speed, five angles45° goes furthest; 20° and 70° tie Mechanics

The angle that throws furthest, and why nobody notices

Forty-five degrees is the answer, and the maximum is so flat that a throw ten degrees off loses almost nothing. Both halves of that are worth drawing.

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27°mgNmg sin θf Mechanics

The slope, and the two directions that make it easy

An inclined plane looks like a harder problem than a flat one. Split the weight into two components chosen to suit the slope and it becomes an easier one.

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before23.001-1.00momentum 5.00energy 9.50after20.3314.33momentum 5.00energy 9.50energy survives too — but only because e = 1 Mechanics

Collisions are easier than forces, and momentum is the reason

Nobody knows what happens inside a collision. Momentum conservation makes that ignorance irrelevant, which is the whole trick — and energy, deliberately, is not conserved.

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00.511.522.5-101positionone wavelength Waves

A wave is a shape that travels, and nothing else does

In a wave on water, no water goes anywhere. What moves is the shape — and separating the two motions is the whole of wave physics.

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sourcesourcesolid: waves arrive in stepbetween them they arrive opposed Waves

When two waves meet, they simply add

Waves pass through each other unchanged and their displacements add point by point. From that one impoverished-sounding rule comes interference, beats, and the evidence that light is a wave at all.

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n = 1fundamentaln = 22× the frequencyn = 33× the frequencyn = 44× the frequency Waves

Only some notes fit, and that is where discreteness comes from

A string clamped at both ends can vibrate at some frequencies and not others. A continuous object producing a whole-number list is the oldest quantisation in physics.

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40°25.4°n = 1n = 1.5some light always reflects as well Optics

The bend at the boundary, and what it is really about

Light changes direction when it changes speed. Snell's law is the geometry of that statement, and it can be derived without knowing anything about light at all.

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FFobjectimageu = 2.44 fv = 1.69 fmagnification -0.69 Optics

What a lens is doing, and why three rays are enough

A lens bends every ray that reaches it. The construction uses three, because three are all that can be drawn without calculation — and any three that meet prove all the rest do.

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020406080020406080incident angle (degrees)critical angle 41.8°beyond this, nothing emergesdashed: no bending at all Optics

The angle past which light cannot leave

Snell's law asks for the sine of an angle greater than one, and no such angle exists. What happens instead is a perfect mirror made out of nothing but a change of speed.

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+ Electromagnetism

Field lines are a choice, not a discovery

Nothing in space is arranged in lines. The lines are a drawing convention — and an unusually good one, because three separate facts about the field survive the translation.

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+lines and arrows are the same fielddrawn two ways Electromagnetism

The field before the lines were drawn on it

A field is a vector attached to every point of space. Drawing it as arrows on a grid is honest and ugly; drawing it as lines is beautiful and throws information away.

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+every line leaves: net flux counts the chargethe shape of the surface never enters the answer Electromagnetism

Counting what comes out, and never looking inside

Draw any closed surface. The field crossing it depends only on the charge enclosed — not on where that charge sits, not on its shape, not on anything outside.

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0123456700.20.40.60.8speedT = 0.5T = 1T = 2T = 4no molecule has the average speed; most are near it Thermodynamics

The speeds in a still room

The air in a quiet room is not still. Every molecule in it is moving at hundreds of metres per second, and temperature is a single number summarising an entire distribution.

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1010145212032104252521061207458109110number of heads1,024 arrangements in total, all equally likelythe middle has 252 of them Thermodynamics

Entropy is a count, and the arrow of time is arithmetic

Nothing in mechanics prefers a direction. Entropy is not a force pushing things toward disorder — it is the observation that some outcomes have vastly more ways of happening than others.

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123400.511.5volumepressure1234net workhot isothermcold isothermadiabatic steps Thermodynamics

The ceiling on every engine, set before it was designed

There is a maximum efficiency no heat engine can exceed, and it depends on nothing but two temperatures. Not the fuel, not the working substance, not the cleverness of the engineer.

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xctlightct′x′here, nowfuturepastunreachableγ = 1.155 — the axes close on the light line together Relativity

Two axes, one speed, and a diagram that does the arguing

Put position across and time up, insist that light travels at forty-five degrees for everyone, and nearly every result in special relativity becomes something to read off rather than derive.

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at restlight goes straight upmovinglight travels 1.25× as farγ = 1.250the ratio is forced by one constant speed Relativity

The clock that has to slow, and why no clock can refuse

One constant speed and one right-angled triangle force a moving clock to tick slower. The argument is Pythagoras, which is what makes it inescapable rather than merely surprising.

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xctsame time, for one observersame time, for the otherABneither slicing is the right one: that is the content of relativity Relativity

Now is a choice of slicing

Two events happening at the same time is not a fact about the events. It is a fact about who is asking, and different observers slice spacetime at different angles.

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Threads running through

themes, not chapters