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Sphere Eversion

4 min read
https://rreusser.github.io/explorations/sphere-eversion/

Topology is the study of the properties of geometric objects which aren’t changed by continuous deformation. A standard low-grade math joke is that toplogists consider a coffee mug and a doughnut equivalent because they’re both torii—(pauses for laughter)—one can be continuously deformed into the other, called a homeomorphism, without cutting or creasing the surface.

Homeomorphism between a doughnut and a mug. Source: Wikipedia

In this post, we play a topological game called eversion. Our objective is simple: turn a sphere inside out without cutting or creasing it. We consider a sphere, though a torus is also an interesting challenge.

That a sphere (specifically the two-sphere S2S^2 embedded in three dimensional space R3mathbb{R}^3 ) can be turned inside out was proved by Stephen Smale in 1957. However the proof is a proof of existence, offering no particular guidance for those hoping to perform the feat.

Circle eversion in two dimensions is impossible. We always get stuck!

We should take a moment to appreciate that the analogous problem of everting a circle in two dimensions is impossible. The figure above illustrates that there’s really nothing to do but introduce loops which we can’t then get rid of. Don’t take my word for it though! The classic video Outside In has an much more involved discussion of what happens when we try.

Since the original proof, a number of realizations of sphere eversion have been discovered, ranging in generality and complexity. This post follows the method of Bednorz and Bednorz from Analytic sphere eversion using ruled surfaces.

Before stepping through the eversion, we lay out our ground rules, of which there are just two: We may not cut the surface, and the surface must always remain smooth. Note that unlike physical objects, self-intersection is permitted.

Bednorz’ Sphere Eversion

We start with a full presentation of the sphere eversion of Bednorz and Bednorz in Analytic sphere eversion using ruled surfaces. It goes by quickly, so we’ll then break it down and try to understand it a bit better. Along the way, you can drag the slider at the top to examine cross-sections.

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Success! But that all happened very quickly. What happens at the top is clearly the key. In some sense, we do simply push one end of the sphere right through the other, but we need some clever tricks to keep the hole at the top smooth.

Bednorz and Bednorz break down the method as follows. As long as nothing topologically interesting happens at the poles of the sphere, we can simply remove them from the equation and focus on a cylindrical band around the equator. All that’s left then is to manipulate the cylindrical band carefully and replace the poles at the end of the process.

The key element of their method is a family of ruled surfaces, or surfaces swept out by a straight line moving through space, which accomplish this task. They propose a family parameterized by time tt . They’re careful to prove the surface remains smooth during the process, but we’ll remain content to get to our destination and visually check the smoothness along the way.

They propose the family of ruled surfaces given by the equations

x=tcos⁡ϕ+psin⁡(n−1)ϕ−hsin⁡ϕy=tsin⁡ϕ+pcos⁡(n−1)ϕ+hcos⁡ϕz=hsin⁡nϕ−(t/n)cos⁡nϕ−qth.
begin{aligned}
x &= t cos phi + p sin (n – 1) phi – h sin phi \
y &= t sin phi + p cos (n – 1) phi + h cos phi \
z &= h sin n phi – (t / n) cos n phi – qth.
end{aligned}

The variable ϕphi parameterizes the polar angle of the cylinder from −π-pi to πpi while hh parameterizes the vertical dimension of the cylinder. They suggest q=2/3q = 2/3 and p=1−∣qt∣p = 1 – |qt| .

Adjust the time parameter tt and observe the shape of the surface. There are two particular things to note. First, the surface always remains smooth, despite self-intersections, and second, the top and bottom of the edges of the cylinder swap places (with a bit of rotation which doesn’t trouble us) as we move from t=−1.5t = -1.5 to t=1.5t = 1.5 .

Note also that although we’ll visualize eversion with n=2n = 2 , the eversion also works for values greater than two.

t = 1.500000
n = 2

The proposed cylindrical ruled surface.

Of course we want to evert a full sphere and not just a cylindrical band, so the remainder of their paper focuses on using stereographic projections to smoothly close the caps of the cylindrical band and maintain the topology of the sphere during the entire process. The full eversion is illustrated above, but let’s now step back through it, taking a bit more care to focus on the region of interest.

And that’s that! I regret that I have nothing novel or nuanced to say about the eversion itself, but my goal here was to explore the visual presentation since videos and images always left me wishing it were a bit more tangible.

There’s no shortage of really great visualizations and resources regarding sphere eversion, among other topics. Below are a few links relevant to both this eversion and the topic in general.

This post is created using idyll and regl. You can find the full article source here.

Comments? Questions? Corrections? Let me know!

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