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{{distinguish|Sphere inversion}}
{{short description|Topological operation of turning a sphere inside-out without creasing}}
] seen from "above"]] ] seen from "above"]]
] ]
]
In ], '''sphere eversion''' is the process of turning a ] inside out in a ]. (The word '']'' means "turning inside out".) Remarkably, it is possible to smoothly and continuously turn a sphere inside out in this way (with possible ]s) without cutting or tearing it or creating any crease. This is surprising, both to non-mathematicians and to those who understand ], and can be regarded as a ]; that is something that, while being true, on first glance seems false.
]

In ], '''sphere eversion''' is the process of turning a ] inside out in a ] (the word '']'' means "turning inside out"). It is possible to smoothly and continuously turn a sphere inside out in this way (allowing ]s of the sphere's surface) without cutting or tearing it or creating any ]. This is surprising, both to non-mathematicians and to those who understand ], and can be regarded as a ]; that is something that, while being true, on first glance seems false.


More precisely, let More precisely, let
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==History== ==History==
An ] for crease-free sphere eversion was first created by {{harvs|txt|authorlink=Stephen Smale|first=Stephen|last= Smale|year= 1957}}. An ] for crease-free sphere eversion was first created by {{harvs|txt|authorlink=Stephen Smale|first=Stephen|last= Smale|year= 1957}}.
It is difficult to visualize a particular example of such a turning, although some ] have been produced that make it somewhat easier. The first example was exhibited through the efforts of several mathematicians, including ] and ], who was blind. On the other hand, it is much easier to prove that such a "turning" exists and that is what Smale did. It is difficult to visualize a particular example of such a turning, although some ] have been produced that make it somewhat easier. The first example was exhibited through the efforts of several mathematicians, including ] and ], who was blind. On the other hand, it is much easier to prove that such a "turning" exists, and that is what Smale did.


Smale's graduate adviser ] at first told Smale that the result was obviously wrong {{harv|Levy|1995}}. Smale's graduate adviser ] at first told Smale that the result was obviously wrong {{harv|Levy|1995}}.
His reasoning was that the ] of the ] must be preserved in such "turning"—in particular it follows that there is no such ''turning'' of '''S'''<sup>1</sup> in '''R'''<sup>2</sup>. But the degrees of the Gauss map for the embeddings ''f'' and &minus;''f'' in '''R'''<sup>3</sup> are both equal to 1, and do not have opposite sign as one might incorrectly guess. The degree of the Gauss map of all immersions of '''S'''<sup>2</sup> in '''R'''<sup>3</sup> is 1, so there is no obstacle. The term "veridical paradox" applies perhaps more appropriately at this level: until Smale's work, there was no documented attempt to argue for or against the eversion of '''S'''<sup>2</sup>, and later efforts are in hindsight, so there never was a historical paradox associated with sphere eversion, only an appreciation of the subtleties in visualizing it by those confronting the idea for the first time. His reasoning was that the ] of the ] must be preserved in such "turning"—in particular it follows that there is no such ''turning'' of '''S'''<sup>1</sup> in '''R'''<sup>2</sup>. But the degrees of the Gauss map for the embeddings ''f'' and &minus;''f'' in '''R'''<sup>3</sup> are both equal to 1, and do not have opposite sign as one might incorrectly guess. The degree of the Gauss map of all immersions of '''S'''<sup>2</sup> in '''R'''<sup>3</sup> is 1, so there is no obstacle. The term "veridical paradox" applies perhaps more appropriately at this level: until Smale's work, there was no documented attempt to argue for or against the eversion of '''S'''<sup>2</sup>, and later efforts are in hindsight, so there never was a historical paradox associated with sphere eversion, only an appreciation of the subtleties in visualizing it by those confronting the idea for the first time.


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Smale's original proof was indirect: he identified (regular homotopy) classes of immersions of spheres with a homotopy group of the ]. Since the homotopy group that corresponds to immersions of <math>S^2 </math> in <math>\R^3</math> vanishes, the standard embedding and the inside-out one must be regular homotopic. In principle the proof can be unwound to produce an explicit regular homotopy, but this is not easy to do. Smale's original proof was indirect: he identified (regular homotopy) classes of immersions of spheres with a homotopy group of the ]. Since the homotopy group that corresponds to immersions of <math>S^2 </math> in <math>\R^3</math> vanishes, the standard embedding and the inside-out one must be regular homotopic. In principle the proof can be unwound to produce an explicit regular homotopy, but this is not easy to do.


There are several ways of producing explicit examples and beautiful ]: There are several ways of producing explicit examples and ]:
] for a description of the video's contents]]
* ]s: these consist of very special homotopies. This is the original method, first done by Shapiro and Phillips via ], later refined by many others. The original half-way model homotopies were constructed by hand, and worked topologically but weren't minimal. The movie created by Nelson Max, over a seven-year period, and based on Charles Pugh's chicken-wire models (subsequently stolen from the Mathematics Department at Berkeley), was a computer-graphics 'tour de force' for its time, and set the bench-mark for computer animation for many years. A more recent and definitive graphics refinement (1980s) is ]s, which is a ] method, and consist of special homotopies (they are shortest paths with respect to ]). In turn, understanding behavior of Willmore energy requires understanding solutions of fourth-order partial differential equations, and so the visually beautiful and evocative images belie some very deep mathematics beyond Smale's original abstract proof. * ]s: these consist of very special homotopies. This is the original method, first done by Shapiro and Phillips via ], later refined by many others. The original half-way model homotopies were constructed by hand, and worked topologically but weren't minimal. The movie created by Nelson Max, over a seven-year period, and based on Charles Pugh's chicken-wire models (subsequently stolen from the Mathematics Department at Berkeley), was a computer-graphics 'tour de force' for its time, and set the bench-mark for computer animation for many years. A more recent and definitive graphics refinement (1980s) is ]s, which is a ] method, and consist of special homotopies (they are shortest paths with respect to ]). In turn, understanding behavior of Willmore energy requires understanding solutions of fourth-order partial differential equations, and so the visually beautiful and evocative images belie some very deep mathematics beyond Smale's original abstract proof.
] for a description of the video's contents]]
* ]'s corrugations: this is a ] method and generic; it takes a homotopy and perturbs it so that it becomes a regular homotopy. This is illustrated in the computer-graphics animation ''Outside In'' developed at the ] under the direction of Silvio Levy, Delle Maxwell and ].<ref>{{cite web|title=Outside In: Introduction|url=http://www.geom.uiuc.edu/docs/outreach/oi/|website=The Geometry Center|accessdate=21 June 2017|archivedate=14 June 1996}}</ref> * ]'s corrugations: this is a ] method and generic; it takes a homotopy and perturbs it so that it becomes a regular homotopy. This is illustrated in the computer-graphics animation ''Outside In'' developed at the ] under the direction of Silvio Levy, Delle Maxwell and ].<ref>{{cite web|title=Outside In: Introduction|url=http://www.geom.uiuc.edu/docs/outreach/oi/|website=The Geometry Center|access-date=21 June 2017}}</ref>
* Aitchison's 'holiverse' (2010): this uses a combination of topological and geometric methods, and is specific to the actual regular homotopy between a standardly embedded 2-sphere, and the embedding with reversed orientation. This provides conceptual understanding for the process, revealed as arising from the concrete structure of the 3-dimensional projective plane and the underlying geometry of the Hopf fibration. Understanding details of these mathematical concepts is not required to conceptually appreciate the concrete eversion that arises, which in essence only requires understanding a specific embedded circle drawn on a torus in 3-space. George Francis suggested the name "holiverse", derived from the word "holistic", since (after some thought) the complete eversion can be conceptually grasped from beginning to end, without the visual aids provided by animation. In spirit, this is closer to the ideas originally suggested by Shapiro, and in practice provides a concrete proof of eversion not requiring the abstraction underlying Smale's proof. This is partially illustrated in a ] computer-graphics animation, again easily found by searching YouTube.
* Combining the above methods, the complete sphere eversion can be described by a set of closed equations giving minimal topological complexity <ref name=sev-eq>{{cite arXiv|title=Analytic sphere eversion with minimum of topological events | arxiv =1711.10466 }}</ref> * Combining the above methods, the complete sphere eversion can be described by a set of closed equations giving minimal topological complexity <ref name=sev-eq>{{cite journal|title=Analytic sphere eversion using ruled surfaces | arxiv =1711.10466 | last1 =Bednorz | first1 =Adam | last2 =Bednorz | first2 =Witold | journal =Differential Geometry and Its Applications | year =2019 | volume =64 | pages =59–79 | doi =10.1016/j.difgeo.2019.02.004 | s2cid =119687494 }} </ref>

==Variations==
* A six-dimensional sphere <math>S^6</math> in seven-dimensional euclidean space <math>\mathbb{R}^7</math> admits eversion.<ref>{{cite book
| last = Goryunov | first = Victor V.
| contribution = Local invariants of mappings of surfaces into three-space
| isbn = 0-8176-3883-0
| pages = 223–255
| publisher = Birkhäuser | location = Boston, Massachusetts
| title = The Arnold–Gelfand mathematical seminars
| year = 1997}}</ref> With an evident case of an 0-dimensional sphere <math>S^0</math> (two distinct points) in a real line <math>\mathbb{R}</math> and described above case of a two-dimensional sphere in <math>\mathbb{R}^3 </math> there are only three cases when sphere <math>S^n</math> embedded in euclidean space <math>\mathbb{R}^{n+1}</math> admits eversion.

==Gallery of eversion steps==
{| class="wikitable" style="margin-left: auto; margin-right: auto; border: none;"
|+Surface plots
|{{multiple image |align= center | header = Ruled model of halfway with quadruple point | width =100 | image1= hw-a.png| caption1=top view|
image2 = hw-b.png| caption2= diagonal view|
image3 = hw-c.png| caption3= side view|direction=|total_width=|alt1=}}
|{{multiple image |align= center | header = Closed halfway | width =100 | image1= morin-a.png| caption1=top view|
image2 = morin-b.png| caption2= diagonal view|
image3 = morin-c.png| caption3= side view|direction=|total_width=|alt1=}}
|{{multiple image |align= center | header = Ruled model of death of triple points | width =100 | image1= Ttw-b.png| caption1=top view|
image2 = Ttw-b1.png| caption2= diagonal view|
image3 = Ttw-b2.png| caption3= side view|direction=|total_width=|alt1=}}
|-
|{{multiple image |align= center | header = Ruled model of end of central intersection loop | width =100 | image1= Ddw-b.png| caption1=top view|
image2 = Ddw-b1.png| caption2= diagonal view|
image3 = Ddw-b2.png| caption3= side view|direction=|total_width=|alt1=}}
| colspan="2" |{{multiple image |align= center | header = Ruled model of last stage | width =100 | image1= Ww-b.png| caption1=top view|
image2 = Ww-b1.png| caption2= diagonal view|
image3 = Ww-b2.png| caption3= side view|direction=|total_width=|alt1=}}
|}



{{multiple image
| align = center
| header = Nylon string open model
| width = 100
| image1 = Q-point.jpg
| caption1 = halfway top
| image2 = Q-point2.jpg
| caption2 = halfway side
| image3 = T-point.jpg
| caption3 = triple death top
| image4 = T-point2.jpg
| caption4 = triple death side
| image5 = D-point.jpg
| caption5 = intersection end top
| image6 = D-point2.jpg
| caption6 = intersection end side
| direction =
| total_width =
| alt1 =
}}




==See also== ==See also==
* ]
* ] * ]


==References== ==References==
{{Reflist}}
* , preprint. arXiv:1008.0916.

===Bibliography===
* , preprint. arXiv:1008.0916.
* John B. Etnyre (2004) Review of "h-principles and flexibility in geometry", {{MathSciNet|id=1982875}}. * John B. Etnyre (2004) Review of "h-principles and flexibility in geometry", {{MathSciNet|id=1982875}}.
* {{Citation | last1=Francis | first1=George K. | title=A topological picturebook | publisher=] | location=Berlin, New York | isbn=978-0-387-34542-0 | mr=2265679 | year=2007}} * {{Citation | last1=Francis | first1=George K. | title=A topological picturebook |title-link=A Topological Picturebook| publisher=] | location=Berlin, New York | isbn=978-0-387-34542-0 | mr=2265679 | year=2007}}
* George K. Francis & ] (1980) "Arnold Shapiro's Eversion of the Sphere", ] 2(4):200&ndash;3. * George K. Francis & ] (1980) "Arnold Shapiro's Eversion of the Sphere", ] 2(4):200&ndash;3.
* {{Citation | last1=Levy | first1=Silvio | title=Making waves | publisher=A K Peters Ltd. | location=Wellesley, MA | isbn=978-1-56881-049-2 | mr=1357900 | year=1995 | chapter=A brief history of sphere eversions | chapterurl=http://www.geom.uiuc.edu/docs/outreach/oi/history.html}} * {{Citation | last1=Levy | first1=Silvio | title=Making waves | publisher=A K Peters Ltd. | location=Wellesley, MA | isbn=978-1-56881-049-2 | mr=1357900 | year=1995 | chapter=A brief history of sphere eversions | chapter-url=http://www.geom.uiuc.edu/docs/outreach/oi/history.html}}
* Max, Nelson (1977) "Turning a Sphere Inside Out", https://www.crcpress.com/Turning-a-Sphere-Inside-Out-DVD/Max/9781466553941 * Max, Nelson (1977) "Turning a Sphere Inside Out", https://www.crcpress.com/Turning-a-Sphere-Inside-Out-DVD/Max/9781466553941 {{Webarchive|url=https://web.archive.org/web/20160304074158/https://www.crcpress.com/Turning-a-Sphere-Inside-Out-DVD/Max/9781466553941 |date=2016-03-04 }}
* Anthony Phillips (May 1966) "Turning a surface inside out", ''Scientific American'', pp.&nbsp;112–120. * Anthony Phillips (May 1966) "Turning a surface inside out", ''Scientific American'', pp.&nbsp;112–120.
* {{Citation | last1=Smale | first1=Stephen | author1-link=Stephen Smale | title=A classification of immersions of the two-sphere | jstor=1993205 | mr=0104227 | year=1958 | journal=] | issn=0002-9947 | volume=90 | pages=281–290 | doi=10.2307/1993205}} * {{Citation | last1=Smale | first1=Stephen | author1-link=Stephen Smale | title=A classification of immersions of the two-sphere | jstor=1993205 | mr=0104227 | year=1958 | journal=] | issn=0002-9947 | volume=90 | issue=2 | pages=281–290 | doi=10.2307/1993205| doi-access=free }}


==External links== ==External links==
* {{Webarchive|url=https://web.archive.org/web/20200711130735/http://torus.math.uiuc.edu/jms/Papers/isama/color/opt2.htm |date=2020-07-11 }}
* , full video (short clip {{deadlink|date=November 2017}})
*
* *
* *
* *
* * The deNeve/Hills sphere eversion: and
* to formalise the proof in the ]

* An of Adam Bednorz and Witold Bednorz method of sphere eversion
==References==
* : A video exploration of sphere eversion, created by ] of ].
{{Reflist}}
{{Portal bar|Mathematics}}


{{DEFAULTSORT:Smale's Paradox}} {{DEFAULTSORT:Smale's Paradox}}
] ]
] ]

Latest revision as of 22:16, 30 June 2024

Not to be confused with Sphere inversion. Topological operation of turning a sphere inside-out without creasing
A Morin surface seen from "above"
Sphere eversion process as described in
Paper sphere eversion and Morin surface
Paper Morin surface (sphere eversion halfway) with hexagonal symmetry

In differential topology, sphere eversion is the process of turning a sphere inside out in a three-dimensional space (the word eversion means "turning inside out"). It is possible to smoothly and continuously turn a sphere inside out in this way (allowing self-intersections of the sphere's surface) without cutting or tearing it or creating any crease. This is surprising, both to non-mathematicians and to those who understand regular homotopy, and can be regarded as a veridical paradox; that is something that, while being true, on first glance seems false.

More precisely, let

f : S 2 R 3 {\displaystyle f\colon S^{2}\to \mathbb {R} ^{3}}

be the standard embedding; then there is a regular homotopy of immersions

f t : S 2 R 3 {\displaystyle f_{t}\colon S^{2}\to \mathbb {R} ^{3}}

such that ƒ0 = ƒ and ƒ1 = −ƒ.

History

An existence proof for crease-free sphere eversion was first created by Stephen Smale (1957). It is difficult to visualize a particular example of such a turning, although some digital animations have been produced that make it somewhat easier. The first example was exhibited through the efforts of several mathematicians, including Arnold S. Shapiro and Bernard Morin, who was blind. On the other hand, it is much easier to prove that such a "turning" exists, and that is what Smale did.

Smale's graduate adviser Raoul Bott at first told Smale that the result was obviously wrong (Levy 1995). His reasoning was that the degree of the Gauss map must be preserved in such "turning"—in particular it follows that there is no such turning of S in R. But the degrees of the Gauss map for the embeddings f and −f in R are both equal to 1, and do not have opposite sign as one might incorrectly guess. The degree of the Gauss map of all immersions of S in R is 1, so there is no obstacle. The term "veridical paradox" applies perhaps more appropriately at this level: until Smale's work, there was no documented attempt to argue for or against the eversion of S, and later efforts are in hindsight, so there never was a historical paradox associated with sphere eversion, only an appreciation of the subtleties in visualizing it by those confronting the idea for the first time.

See h-principle for further generalizations.

Proof

Smale's original proof was indirect: he identified (regular homotopy) classes of immersions of spheres with a homotopy group of the Stiefel manifold. Since the homotopy group that corresponds to immersions of S 2 {\displaystyle S^{2}} in R 3 {\displaystyle \mathbb {R} ^{3}} vanishes, the standard embedding and the inside-out one must be regular homotopic. In principle the proof can be unwound to produce an explicit regular homotopy, but this is not easy to do.

There are several ways of producing explicit examples and mathematical visualization:

Minimax sphere eversion; see the video's Wikimedia Commons page for a description of the video's contents
  • Half-way models: these consist of very special homotopies. This is the original method, first done by Shapiro and Phillips via Boy's surface, later refined by many others. The original half-way model homotopies were constructed by hand, and worked topologically but weren't minimal. The movie created by Nelson Max, over a seven-year period, and based on Charles Pugh's chicken-wire models (subsequently stolen from the Mathematics Department at Berkeley), was a computer-graphics 'tour de force' for its time, and set the bench-mark for computer animation for many years. A more recent and definitive graphics refinement (1980s) is minimax eversions, which is a variational method, and consist of special homotopies (they are shortest paths with respect to Willmore energy). In turn, understanding behavior of Willmore energy requires understanding solutions of fourth-order partial differential equations, and so the visually beautiful and evocative images belie some very deep mathematics beyond Smale's original abstract proof.
Sphere eversion using Thurston's corrugations; see the video's Wikimedia Commons page for a description of the video's contents
  • Thurston's corrugations: this is a topological method and generic; it takes a homotopy and perturbs it so that it becomes a regular homotopy. This is illustrated in the computer-graphics animation Outside In developed at the Geometry Center under the direction of Silvio Levy, Delle Maxwell and Tamara Munzner.
  • Combining the above methods, the complete sphere eversion can be described by a set of closed equations giving minimal topological complexity

Variations

  • A six-dimensional sphere S 6 {\displaystyle S^{6}} in seven-dimensional euclidean space R 7 {\displaystyle \mathbb {R} ^{7}} admits eversion. With an evident case of an 0-dimensional sphere S 0 {\displaystyle S^{0}} (two distinct points) in a real line R {\displaystyle \mathbb {R} } and described above case of a two-dimensional sphere in R 3 {\displaystyle \mathbb {R} ^{3}} there are only three cases when sphere S n {\displaystyle S^{n}} embedded in euclidean space R n + 1 {\displaystyle \mathbb {R} ^{n+1}} admits eversion.

Gallery of eversion steps

Surface plots
Ruled model of halfway with quadruple pointtop viewdiagonal viewside view Closed halfwaytop viewdiagonal viewside view Ruled model of death of triple pointstop viewdiagonal viewside view
Ruled model of end of central intersection looptop viewdiagonal viewside view Ruled model of last stagetop viewdiagonal viewside view


Nylon string open modelhalfway tophalfway sidetriple death toptriple death sideintersection end topintersection end side


See also

References

  1. ^ Bednorz, Adam; Bednorz, Witold (2019). "Analytic sphere eversion using ruled surfaces". Differential Geometry and Its Applications. 64: 59–79. arXiv:1711.10466. doi:10.1016/j.difgeo.2019.02.004. S2CID 119687494.
  2. "Outside In: Introduction". The Geometry Center. Retrieved 21 June 2017.
  3. Goryunov, Victor V. (1997). "Local invariants of mappings of surfaces into three-space". The Arnold–Gelfand mathematical seminars. Boston, Massachusetts: Birkhäuser. pp. 223–255. ISBN 0-8176-3883-0.

Bibliography

External links

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