Hairy Ball Theorem

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## Counting zeros

## Application to computer graphics

## Lefschetz connection

## Corollary

## Higher dimensions

## See also

## Notes

## References

## Further reading

## External links

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

Hairy Ball Theorem

The **hairy ball theorem** of algebraic topology (sometimes called the **hedgehog theorem** in Europe)^{[1]} states that there is no nonvanishing continuous tangent vector field on even-dimensional *n*-spheres.^{[2]}^{[3]} For the ordinary sphere, or 2-sphere, if *f* is a continuous function that assigns a vector in **R**^{3} to every point *p* on a sphere such that *f*(*p*) is always tangent to the sphere at *p*, then there is at least one pole, a point where the field vanishes (a *p* such that *f*(*p*) = **0).**

The theorem was first proved by Henri Poincaré for the 2-sphere in 1885,^{[4]} and extended to higher dimensions in 1912 by Luitzen Egbertus Jan Brouwer.^{[5]}

The theorem has been expressed colloquially as "you can't comb a hairy ball flat without creating a cowlick" or "you can't comb the hair on a coconut".^{[6]}

Every zero of a vector field has a (non-zero) "index", and it can be shown that the sum of all of the indices at all of the zeros must be two, because the Euler characteristic of the 2-sphere is two. Therefore, there must be at least one zero. This is a consequence of the Poincaré-Hopf theorem. In the case of the torus, the Euler characteristic is 0; and it is possible to "comb a hairy doughnut flat". In this regard, it follows that for any compact regular 2-dimensional manifold with non-zero Euler characteristic, any continuous tangent vector field has at least one zero.

A common problem in computer graphics is to generate a non-zero vector in **R**^{3} that is orthogonal to a given non-zero one. There is no single continuous function that can do this for all non-zero vector inputs. This is a corollary of the hairy ball theorem. To see this, consider the given vector as the radius of a sphere and note that finding a non-zero vector orthogonal to the given one is equivalent to finding a non-zero vector that is tangent to the surface of that sphere where it touches the radius. However, the hairy ball theorem says there exists no continuous function that can do this for every point on the sphere (equivalently, for every given vector).

There is a closely related argument from algebraic topology, using the Lefschetz fixed-point theorem. Since the Betti numbers of a 2-sphere are 1, 0, 1, 0, 0, ... the *Lefschetz number* (total trace on homology) of the identity mapping is 2. By integrating a vector field we get (at least a small part of) a one-parameter group of diffeomorphisms on the sphere; and all of the mappings in it are homotopic to the identity. Therefore, they all have Lefschetz number 2, also. Hence they have fixed points (since the Lefschetz number is nonzero). Some more work would be needed to show that this implies there must actually be a zero of the vector field. It does suggest the correct statement of the more general Poincaré-Hopf index theorem.

A consequence of the hairy ball theorem is that any continuous function that maps an even-dimensional sphere into itself has either a fixed point or a point that maps onto its own antipodal point. This can be seen by transforming the function into a tangential vector field as follows.

Let *s* be the function mapping the sphere to itself, and let *v* be the tangential vector function to be constructed. For each point *p*, construct the stereographic projection of *s*(*p*) with *p* as the point of tangency. Then *v*(*p*) is the displacement vector of this projected point relative to *p*. According to the hairy ball theorem, there is a *p* such that *v*(*p*) = **0**, so that *s*(*p*) = *p*.

This argument breaks down only if there exists a point *p* for which *s*(*p*) is the antipodal point of *p*, since such a point is the only one that cannot be stereographically projected onto the tangent plane of *p*.

The connection with the Euler characteristic ? suggests the correct generalisation: the 2*n*-sphere has no non-vanishing vector field for . The difference between even and odd dimensions is that, because the only nonzero Betti numbers of the *m*-sphere are b_{0} and b_{m}, their alternating sum ? is 2 for *m* even, and 0 for *m* odd.

**^**Renteln, Paul (2013).*Manifolds, Tensors, and Forms: An Introduction for Mathematicians and Physicists*. Cambridge Univ. Press. p. 253. ISBN 978-1107659698.**^**Burns, Keith; Gidea, Marian (2005).*Differential Geometry and Topology: With a View to Dynamical Systems*. CRC Press. p. 77. ISBN 1584882530.**^**Schwartz, Richard Evan (2011).*Mostly Surfaces*. American Mathematical Society. pp. 113-114. ISBN 978-0821853689.**^**Poincaré, H. (1885), "Sur les courbes définies par les équations diff ?erentielles",*Journal de Mathématiques Pures et Appliquées*,**4**: 167-244**^**Georg-August-Universität Göttingen Archived 2006-05-26 at the Wayback Machine - L.E.J. Brouwer. Über Abbildung von Mannigfaltigkeiten / Mathematische Annalen (1912) Volume: 71, page 97-115; ISSN: 0025-5831; 1432-1807/e, full text**^**Richeson, David S. (23 July 2019).*Euler's gem : the polyhedron formula and the birth of topology*(New Princeton science library ed.). Princeton. p. 5. ISBN 978-0691191997.

- Eisenberg, Murray; Guy, Robert (1979), "A Proof of the Hairy Ball Theorem",
*The American Mathematical Monthly*,**86**(7): 571-574, doi:10.2307/2320587, JSTOR 2320587

- Jarvis, Tyler; Tanton, James (2004), "The Hairy Ball Theorem via Sperner's Lemma",
*American Mathematical Monthly*,**111**(7): 599-603, doi:10.1080/00029890.2004.11920120, JSTOR 4145162, S2CID 29784803 - Reich, Henry (2011),
*One-Minute Math: Why you can't comb a hairy ball*, New ScientistTV - Richeson, David S. (2008), "Combing the Hair on a Coconut",
*Euler's Gem: The Polyhedron Formula and the Birth of Topology*, Princeton University Press, pp. 202-218, ISBN 978-0-691-12677-7

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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