Computation

The spiral that measures its own circle

Let a ray turn steadily while a point moves steadily out along it, and the point draws Archimedes' spiral. Distance from the centre is then proportional to angle, so dividing a length divides an angle in any ratio. The spiral's second power is stranger: the tangent at the end of the first turn cuts off, on a line through the centre, a straight length exactly equal to the circumference of the circle through that end — a curved length laid out straight, and with it the circle squared. The catch is the tangent itself.

Worth reading first: A curve that divides any angle · The mark that changes what is reachable.

A curve that divides any angle found an instrument in a curve: Hippias’s quadratrix, drawn by two uniform motions, turns heights into angles and so divides any angle in any ratio, and its foot sits at 2/π2/\pi of the side, a length that squares the circle. It mentioned, in passing, that the quadratrix was not the only such curve. The other famous one is older in its full treatment and more surprising in how it works.

Archimedes wrote On Spirals around 225 BC, crediting the idea to his friend Conon of Samos. The curve is traced by a point that moves steadily outward along a ray while the ray turns steadily about its end. After one full turn the point has travelled out a fixed distance. The distance from the centre is then proportional to the angle turned:

r=aθ.r = a\theta.

That alone makes it an angle divider, exactly as the quadratrix is. But the spiral’s more remarkable property is carried not by its points but by its tangent, and it gives a way of turning the curved length of a circle into a straight one.

The spiral's tangent lays the circumference out straight. Spiral r = aθ to θ = 6.2832; tangent at P meets the perpendicular through O at T with OT = 6.28319 = OP × θ = 6.28319.
Fig. 1 The spiral after one full turn, the tangent at its end P (green), and the line through the centre O at right angles to OP, which the tangent meets at T; the circle through P is drawn faint. OT = 6.2832 and OP = 1.0000: OT is 2π times OP, the whole circumference of the circle through P — a curved length laid out straight by the tangent.

In the figure, the spiral completes one turn and ends at PP, at distance 11 from the centre OO. The tangent to the spiral at PP is drawn, and it crosses the line through OO perpendicular to OPOP at a point TT. The length OTOT comes out at 6.28326.2832: 2π2\pi times OPOP, the circumference of the circle of radius OPOP. The spiral has laid the circle’s circumference out along a straight line.

Distance and angle are one quantity

The curve is easiest to understand by watching it being drawn.

Archimedes' spiral, traced by a turning ray and a point moving out along it. A circle, 8 positions of a turning ray, the point on each at distance equal to the fraction of the turn, and the spiral through them.
Fig. 2 A ray turns steadily once round while a point moves steadily out along it, from the centre to the circle, in the same time. At each eighth of the turn the ray (blue) and the point (orange) are drawn, and the points trace Archimedes’ spiral. The point’s distance from the centre is the fraction of the turn completed.

At an eighth of the turn the point is an eighth of the way out; at three eighths, three eighths of the way; at the end of the turn, all the way out to the circle. Each point’s distance from the centre and its angle round the centre are the same number in two units. The figure checks, at every drawn instant, that the distance equals the fraction of the turn completed.

This is the property the quadratrix had, with a different pairing: there, height was proportional to angle; here, distance from the centre is. Nothing about the curve needs a coordinate system: it is defined entirely by two rates, one of turning and one of moving out, and every property below follows from their fixed ratio. The spiral’s version is more natural in one respect. The quadratrix is drawn inside a square and covers only angles up to a right angle. The spiral covers a whole turn, and continued, as many turns as desired.

Dividing an angle by dividing a length

Given the spiral, dividing any angle in any ratio is a matter of dividing a length.

Cutting a 240° angle into 3 with Archimedes' spiral. Archimedes' spiral, an angle of 240 degrees meeting it at P, OP divided into 3, and the circles through the divisions meeting the spiral on the dividing arms.
Fig. 3 An angle of 240° with its arm meeting the spiral at P. The distance OP is divided into three equal parts, a compass-and-straightedge step, and circles through the division points (dashed) meet the spiral where the arms dividing the angle cross it — at 80° and 160°, checked against the angles themselves.

Draw the angle with one arm along the spiral’s starting direction. Its other arm meets the spiral at a point PP, and the distance OPOP is proportional to the angle. Divide OPOP into three equal parts — the straightedge buys nothing and its neighbours show that compass and straightedge divide a length into any number of equal parts. Draw circles about OO through the division points. Each circle meets the spiral at a point whose distance from OO is one or two thirds of OPOP, and so whose angle is one or two thirds of the given angle. The rays to those points trisect the angle.

The same works for any ratio a length can be cut in, and for angles beyond a right angle, which the quadratrix cannot reach — the figure trisects an angle of 240°240°. The trisection problem that no compass and straightedge can solve in general is here reduced to a step they can do, with the spiral supplying the translation between length and angle.

The tangent that unrolls the circle

The spiral’s own proof of its rectifying property uses one fact about tangents to curves given by an angle-to-distance rule.

For a curve described by its distance rr from OO as a function of the angle θ\theta, the tangent at a point meets the line through OO perpendicular to the radius at a distance

OT=r2 dr/dθ OT = \frac{r^2}{\,dr/d\theta\,}

from OO — the polar subtangent. For the spiral, r=aθr = a\theta and dr/dθ=adr/d\theta = a, so

OT=(aθ)2a=aθ⋅θ=rθ.OT = \frac{(a\theta)^2}{a} = a\theta \cdot \theta = r\theta.

And rθr\theta is the length of the arc of the circle of radius rr through the angle θ\theta. At the end of one full turn, θ=2π\theta = 2\pi, and OT=2πrOT = 2\pi r — the whole circumference.

The spiral's tangent after 0.5 of a turn. Spiral r = aθ to θ = 3.1416; tangent at P meets the perpendicular through O at T with OT = 1.57080 = OP × θ = 1.57080.
Fig. 4 The same construction after half a turn. OP = 0.5 and the tangent meets the perpendicular through O at T with OT = 1.5708 = OP × π: the length of the half-circle of radius OP, laid out straight.

The relation holds at every point, not only at the end of a turn. After half a turn the point is at distance 12\tfrac12, and the tangent cuts off a length π⋅12=1.5708\pi \cdot \tfrac12 = 1.5708: the half-circumference of the circle through it. The figures compute the tangent from the curve’s direction at the point, intersect it with the perpendicular, and check that the length is the arc to within a billionth.

Archimedes proved the full-turn case as Propositions 18 to 20 of On Spirals, without derivatives, by an argument that approaches the tangent from both sides and shows that any other line through PP either cuts the spiral or misses the required length. His proofs of the preliminary propositions use verging constructions — the sliding-mark step of the mark that changes what is reachable — which is one reason the spiral belongs in the same family of instruments as the marked ruler.

Why the tangent knows the arc

The formula hides a picture that makes the result almost obvious. Follow the point for a moment longer, as the ray turns through a tiny angle dθd\theta. The point moves outward by a dθa\,d\theta, because the outward speed is fixed. It also moves sideways, round the centre, by r dθr\,d\theta, because a point at distance rr turning through dθd\theta sweeps an arc of that length. Its motion is the combination of the two, and the tangent points along that combination.

So the tangent makes a small right triangle with the radius: its side along the radius is a dθa\,d\theta and its side across the radius is r dθr\,d\theta. The large triangle OPTOPT — right-angled at OO, with one side along the radius and one across it — is similar to the small one, because the tangent is the hypotenuse of both. Similar triangles have proportional sides:

OTOP=r dθa dθ=ra=θ.\frac{OT}{OP} = \frac{r\,d\theta}{a\,d\theta} = \frac{r}{a} = \theta.

So OT=θ⋅OP=rθOT = \theta \cdot OP = r\theta, the arc of radius rr through angle θ\theta. The tangent’s slope records the ratio of sideways to outward motion, and for this curve that ratio is the angle itself. At the end of a full turn the angle is 2π2\pi, and the tangent triangle is 2π2\pi times as tall as it is wide.

Squaring the circle from the tangent

Once a straight segment equal to the circumference is in hand, the circle can be squared with compass and straightedge alone.

The area of a circle of radius rr is half its circumference times its radius — the observation a circle unrolled made by cutting the disc into rings and laying them out as a triangle of height rr and base 2πr2\pi r. So a rectangle with sides OT/2=πrOT/2 = \pi r and rr has the circle’s area. Converting a rectangle into a square of equal area is a classical compass-and-straightedge step: the square’s side is the geometric mean of the rectangle’s sides, found with a semicircle.

The spiral therefore squares the circle, and it does so more directly than the quadratrix, which produced 2/π2/\pi and needed a proportion to invert it. What the compass could not supply was a straight length equal to a curved one. The spiral supplies it through its tangent, and the rest is Euclid.

A third of the circle, by exhaustion

Archimedes found the area inside the first turn too, and the argument is a model of the method later called exhaustion.

The first turn of the spiral encloses a third of the circle. First turn of Archimedes' spiral with 12 inscribed and circumscribed sectors: 0.91993 < area < 1.18173; π/3 = 1.04720.
Fig. 5 The region inside the first turn of the spiral, squeezed between twelve sectors that fit inside it (solid) and twelve that cover it (light): together they give 0.9199 < area < 1.1817, and the gap is exactly one sector of the whole circle, π/12. The gap vanishes as the sectors are cut finer, and the only number caught between every pair of bounds is π/3: the first turn encloses a third of the circle through its end.

Cut the full turn into nn equal angles. In each, the spiral’s distance from OO runs from aθka\theta_k to aθk+1a\theta_{k+1}, so the region inside the spiral in that angle contains a circular sector of the smaller radius and is contained in one of the larger. The sectors’ areas are 12r2 Δθ\tfrac12 r^2\,\Delta\theta, and because the radii grow linearly, their sums are sums of squares: ∑k2\sum k^2, which Archimedes knew in closed form. The inscribed and circumscribed totals differ by exactly one sector of the full circle, π/n\pi/n when the circle has radius 11, so the gap shrinks to nothing, and the only value both can approach is

13 πr2.\frac{1}{3}\,\pi r^2.

The first turn encloses exactly a third of the circle through its end. The computation is the sum 12∫r2 dθ=12a2∫02πθ2 dθ\tfrac12\int r^2\,d\theta = \tfrac12 a^2 \int_0^{2\pi} \theta^2\,d\theta in modern notation — the polar area formula of an area measured by walking round it — and Archimedes carried it out eighteen centuries before that notation, with sums of squares and a double bound.

The catch: the tangent is not a compass step

Every construction above depends on having the spiral drawn. That is the same objection Sporus raised against the quadratrix: to draw the curve, one must already coordinate a turning motion with an outward one at the exact right rates, which presupposes the very ratio between straight and curved that the curve is used to find.

The spiral adds a second objection, which the quadratrix does not face. The rectification needs the tangent at PP. Drawing a tangent to a circle is a compass-and-straightedge step; drawing a tangent to the spiral is not. There is no finite sequence of circles and lines that produces it from the spiral’s points alone, because the tangent’s direction depends on the rate at which the curve is turning outward — a derivative — and a derivative is a limit. Ancient geometers could characterise the tangent, as Archimedes did, but not construct it from the curve by the permitted operations.

Pappus of Alexandria, writing about 340 AD, sorted problems by the instruments they need: plane problems, solved with lines and circles; solid problems, which need conic sections; and linear problems, which need other curves, among them the quadratrix and the spiral. He held that a problem should be solved with the simplest instrument that can do it, and regarded solving a plane or solid problem with a spiral as a fault of method. By his classification the rectification of the circle is irreducibly linear, and later mathematics — the cube that will not double and Lindemann’s proof that π\pi is transcendental — showed that he was right: no conic, and no finite algebraic construction, reaches π\pi.

The same objection, twice

The quadratrix was criticised on two counts. Sporus complained that drawing it presupposes the ratio it is meant to find, since the two motions must finish together; and that its foot, the point on the base that carries 2/π2/\pi, is not actually traced by the motions at all — at the final instant the radius and the falling line coincide, and the crossing that defines the foot is a limit, not a crossing.

The spiral answers the first complaint no better: it too needs a turning motion and an outward motion in a fixed ratio. And its answer to the second is to move the difficulty rather than remove it. The spiral’s end point PP is traced honestly, but the length that matters, OTOT, is carried by the tangent, and a tangent is a limit of secants. Both curves deliver π\pi only through a limit — the quadratrix at its foot, the spiral at its tangent — and that is no coincidence. π\pi is transcendental, so no finite sequence of algebraic operations reaches it; any construction that does must contain an infinite process somewhere, and the only question is where it is hidden.

The comparison is instructive about what a construction is. The price of a construction counted the steps of compass-and-straightedge constructions and asked for the fewest; a construction with a transcendental curve has a step that no count can price, because it is not a finite operation at all.

Other spirals, other lengths

The spiral whose distance grows in proportion to its angle is not the only spiral with a useful tangent. In the equiangular or logarithmic spiral, r=ebθr = e^{b\theta}, the distance grows in proportion to itself, and the tangent makes the same angle with the radius at every point — the property that shows up in shells and in the growth patterns of plants, and the curve that the rectangle that eats itself approximates by quarter-circles when a golden rectangle is cut into squares over and over. Where Archimedes’ spiral adds a fixed distance for each turn, the equiangular spiral multiplies by a fixed factor, so it looks the same at every scale.

Evangelista Torricelli found in 1645 that this spiral, although it winds round its centre infinitely many times as it approaches it, has a finite length from any point in to the centre: the length is the distance from the centre divided by the cosine of the constant angle. That was one of the first rectifications of a curve in the seventeenth century, when finding a curve’s length was believed by many to be impossible in general. The two spirals divide the labour between them: Archimedes’ spiral rectifies circles, and the equiangular spiral is rectified by a formula in its own terms.

What the figures can and cannot show

The curves are computed, not drawn by motion. Each point of the spiral is placed by its formula; the figures check the proportionality of distance and angle at every drawn instant, and check each claimed division and each claimed length against the angle or arc it is about.

The tangent is computed from the derivative. The figures find the tangent’s direction from the rate of change of the curve’s position, which is exactly the step no compass supplies. They verify Archimedes’ relation; they do not construct the tangent by the ancient means, because there is none.

The area is bracketed at one fineness. Twelve sectors pin the area between 0.920.92 and 1.181.18; the claim that π/3\pi/3 is the only number between every such pair is the argument, and the figure shows one stage of it.

Still open: what a curve can reach

Adding a curve to the instruments enlarges the set of reachable lengths, and for algebraic curves there is a measure of how much: two instruments with one reach found that conics reach exactly the numbers whose degree is built from twos and threes. For transcendental curves like the spiral and the quadratrix, no such measure exists. The spiral reaches π\pi, and every length obtained from π\pi and the constructible numbers by the field operations; it reaches the division of every angle in every rational ratio, and so the sines and cosines of every rational multiple of any given angle.

What else it reaches is not characterised. Whether, for instance, the spiral combined with compass and straightedge can construct ee, or 23\sqrt[3]{2}, or the side of a regular heptagon from a given unit — the second two are algebraic, and reachable by conics, but not obviously by this curve, since the spiral turns lengths into angles and back without solving cubic equations — is not settled by any general theorem. The theory of constructions with transcendental instruments has no analogue of the degree that settles the algebraic case, and each such question has to be answered, if at all, by an argument of its own.

A curve that carries a ratio

The habit worth keeping is to ask what an instrument encodes.

A compass encodes equal distances; a straightedge encodes collinearity; a marked ruler encodes a fixed length that can slide. The spiral encodes the ratio between a straight motion and a turning one, and every one of its powers — dividing angles, rectifying the circle, squaring it, enclosing a third of it — is that ratio read off in a different way. The spiral does not compute π\pi; it contains it, built in by the rule that draws it, and each construction merely points to where it already is.

What links here

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Named objects

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Angle trisectionArchimedean spiralConstructible numberMethod of exhaustionPiSquaring the circleTangentTranscendence