Concept

Sphere

The set of points at a fixed distance from a centre, in any number of dimensions. Its defining property in topology is that it separates: a sphere in n-dimensional space cuts the complement into exactly two pieces, and that is true in every dimension whether or not the sphere sits tamely.

Named by 13 essays across 4 fields — each of them below, with the objects they name alongside it.

A ray through a knotted tube, crossing it 5 times. A closed surface in space — a tube round a trefoil knot — with a point, a ray from it and every crossing of the surface marked; the parity of the count says which side of the surface the point is on.

Two pieces, in every dimension

A closed curve cuts the plane in two. A closed curve in space cuts nothing at all, and it takes a closed surface to do the job — which is the shape of the general theorem, and the reason the word "dimension" means anything.

topology · Jordan curve
Alexander's horned sphere at stage 3. A tree of clasped pairs of horns, 7 of them, each pair's two circles passing once through the other's disc; the horns shrink geometrically and their tips converge.

A ball whose outside is not one

Alexander's sphere separates space into two pieces, exactly as the theorem promises. Its inside is an ordinary ball. Its outside is not, and the obstruction is a tree of clasped horns whose tips never stop.

topology · Jordan curve
Two inversions, and the number four points agree on. Four points, their images after one inversion and after a second in a different circle, with the cross-ratio computed at each stage; it is conjugated once and restored twice.

The number four points agree on

One inversion is a reflection and reverses orientation. Two of them compose to a motion, and what that motion leaves alone is a single number computed from any four points.

geometry · Inversion
Sliding one square past another. 4 stages of a slide in which two labelled squares inside a larger one exchange positions without ever overlapping. The larger square's boundary is the base point throughout, and the exchange is what makes the composition commutative.

Why the second group commutes

Replace loops by spheres and the same construction gives a second homotopy group. It is always commutative, and the reason is not a fact about spheres or about any space — it is a two-line argument about any set carrying two compatible operations.

topology · Homotopy
A circle stays a circle, unless it meets the pole. 3 circles on a sphere beside their stereographic images in the plane, which are circles, together with one circle through the projection point whose image is a straight line.

Angles survive and areas do not

Stereographic projection takes every circle on the sphere to a circle or a line, and every crossing angle to itself. It does both exactly, with no approximation anywhere, and it destroys area so thoroughly that a patch near the pole can be a thousand times its neighbour's size.

topology · Stereographic projection
The six regular 4-polytopes, and an alternating sum of 0. A table of the six regular polytopes in four dimensions with their numbers of vertices, edges, faces and cells and the alternating sum, which is zero for each.

Zero in four dimensions

Corners minus edges plus faces is two for every solid. One dimension up, corners minus edges plus faces minus cells is zero for every one of the six regular four-dimensional solids, from the five-cell to the six-hundred-cell, and for every other convex solid in four dimensions. The alternating sum does not break when the dimension rises: it alternates, two in odd dimensions and zero in even ones, because it is measuring a sphere and not a solid.

topology · Euler characteristic
The largest value on each plane, over every direction of space. A longitude–latitude map of directions u in three dimensions, each shaded by the largest value of xᵀAx on the plane perpendicular to u. The smallest such value is the middle eigenvalue 1.829, reached at ±v₁; the largest is 3.622, reached along a great circle.

The highest point on the sphere is an eigenvalue

For a symmetric matrix, walk a unit arrow over every direction and record the value of xᵀAx. The highest value reached is the largest eigenvalue, the lowest is the smallest, and every eigenvalue in between is a saddle height, a minimum of maxima. From that one description comes a theorem no formula for the roots could give: delete a row and its column, and every eigenvalue of what is left sits between two of the original's.

algebra · Eigenvectors
How much of a sphere lies near its equator. Curves of the share of the sphere within ε of the equator against ε, for spheres in 3, 10, 100, 1000 dimensions: a straight line in three dimensions, a near step in a thousand.

A sphere that is nearly all equator

On an ordinary globe, the band within a tenth of the radius of the equator holds a tenth of the surface. On a sphere in a thousand dimensions the same band holds 99.85% of it, and the band of a fifth holds all but about two parts in ten billion. Almost every point of a high-dimensional sphere is near every equator at once — and so any function that cannot change quickly is, over almost all of the sphere, almost constant.

probability · Concentration
The 9 mirrors of the octahedral group, cutting the sphere into 48 triangles. A sphere crossed by the 9 great circles of the octahedral group's mirror planes, dividing it into 48 triangles with one shaded.

Three mirrors make every solid

Every symmetry of a regular solid, reflections included, is produced by just three mirrors meeting at its centre, reflected in one another over and over — a kaleidoscope. Put a single point between the three mirrors and its reflections are the corners of a solid: the regular solid itself if the point sits in a corner, and every one of its truncated and expanded relatives if it sits anywhere else.

geometry · Regular polyhedra
Bands of a sphere and of its cylinder, cut by the same planes. A unit sphere inside its cylinder with 3 horizontal bands; each sphere band has area 1.885, 1.885, 1.885, equal to the cylinder band of the same height.

A band of a sphere is a band of its cylinder

Cut a sphere with two parallel planes and the band between them has exactly the area of the band the same planes cut from the cylinder wrapped round the sphere — whatever the band's latitude. Near the equator the sphere's band is wide and nearly upright; near a pole it is narrow and nearly flat; and the two effects cancel exactly. Archimedes proved it, wanted it on his tomb, and it gives the area of the sphere, the only honest way to pick a random point on it, and a map on which no country is the wrong size.

geometry · Circle area
The volume of the unit ball and the area of its sphere, dimension by dimension. Unit ball volumes for dimensions 0 to 20, largest at 5 (5.2638); sphere areas largest at 7 (33.0734).

The ball that is largest in five dimensions

A disc of radius one has area π, a ball of radius one volume 4π/3, and in each further dimension the unit ball grows — until five, where its volume is 5.264, after which it shrinks towards nothing. The recursion that shows it is the ring dissection of the disc, done one dimension at a time, and the shrinking is not the ball getting small: it is almost all of a high-dimensional cube lying outside the ball, and almost all of the ball lying in a thin rind at its surface.

geometry · Circle area
An astrolabe is a stereographic projection in brass. Latitude 52°: 16 engraved curves, worst departure from a circle 8.88e-15; altitude-circle formulas within 2.2e-16; Cancer radius 0.6564, Capricorn 1.5235 of the equator's.

An instrument that computes with circles

An astrolabe is a stereographic projection of the sky cut in brass. Because the projection sends circles to circles, every line on it can be drawn with compasses, and turning the star map over the plate is a rotation that answers questions in spherical astronomy without a single calculation. Of the lines medieval makers engraved, one family is not a circle on the sphere — and the arcs they drew for it miss the truth by a third of a millimetre.

topology · Stereographic projection
Two valleys for sixteen charges. N = 16: 92.911655 (48 starts), 92.920354 (12 starts).

Valleys a search cannot count

Let equal charges on a sphere push each other apart from a random start, and they settle into an arrangement where nothing moves. Up to fifteen charges every start settles into the same one. Sixteen is the first number with two, a hundredth of a unit apart in energy; by fifty-two there are at least four, and for fifty-six charges only one start in ten finds the lowest. The other valleys sit a few parts in a million above it, and nothing in the arrangement a search returns says whether it is the bottom.

geometry · Regular polyhedra

Named alongside it

The objects these essays reach for when they reach for this one.

DimensionEuler characteristicGroupProjectionAreaConformalHomeomorphismHypercubeInversionJordan curveKnotMobius transformation

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