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#redirect [[Möbius strip]]

==Properties==
[[File:Moebiusband-1s.svg|thumb|once cut Möbius strip: one non Möbius strip]]
[[File:Moebiusband-2s.svg|thumb|twice cut Möbius strip: one Möbius strip (purple), one non Möbius strip]]
The Möbius strip has several curious properties. A line drawn starting from the seam down the middle meets back at the seam, but at the other side. If continued, the line meets the starting point, and is double the length of the original strip. This single continuous curve demonstrates that the Möbius strip has only one [[Boundary (topology)|boundary]].

Cutting a Möbius strip along the center line with a pair of scissors yields one long strip with two full twists in it, rather than two separate strips; the result is not a Möbius strip. This happens because the original strip only has one edge that is twice as long as the original strip.  Cutting creates a second independent edge, half of which was on each side of the scissors. Cutting this new, longer, strip down the middle creates two strips wound around each other, each with two full twists.

If the strip is cut along about a third of the way in from the edge, it creates two strips: One is a thinner Möbius strip – it is the center third of the original strip, comprising one-third of the width and the same length as the original strip. The other is a longer but thin strip with two full twists in it – this is a [[neighbourhood (mathematics)|neighborhood]] of the edge of the original strip, and it comprises one-third of the width and twice the length of the original strip.

Other analogous strips can be obtained by similarly joining strips with two or more half-twists in them instead of one. For example, a strip with three half-twists, when divided lengthwise, becomes a twisted strip tied in a [[trefoil knot]]. (If this knot is unravelled, the strip has eight half-twists.)  A strip with ''N'' half-twists, when bisected, becomes a strip with ''N'' + 1 full twists.  Giving it extra twists and reconnecting the ends produces figures called [[paradromic ring]]s.

== Geometry and topology ==
[[File:Fiddler crab mobius strip.gif|thumb|An object that existed in a mobius-strip-shaped universe would be indistinguishable from its own mirror image – this fiddler crab's larger claw switches between left to right with every circulation. It is not impossible that the universe may have this property, see [[Non-orientable wormhole]] ]]
[[File:MöbiusStripAsSquare.svg|thumb|To turn a [[rectangle]] into a Möbius strip, join the edges labelled ''A'' so that the directions of the arrows match.]]

One way to represent the Möbius strip as a subset of three-dimensional Euclidean space is using the parametrization:

:<math>x(u,v)= \left(1+\frac{v}{2} \cos \frac{u}{2}\right)\cos u</math>

:<math>y(u,v)= \left(1+\frac{v}{2} \cos\frac{u}{2}\right)\sin u</math>

:<math>z(u,v)= \frac{v}{2}\sin \frac{u}{2}</math>

where <math>0 \le u< 2\pi</math> and <math>-1 \le v\le 1</math>. This creates a Möbius strip of width 1 whose center circle has radius 1, lies in the <math>xy</math>-plane and is centered at <math>(0, 0, 0)</math>. The parameter <math>u</math> runs around the strip while <math>v</math> moves from one edge to the other.

In [[cylindrical coordinates|cylindrical polar coordinates]] <math>(r, \theta, z)</math>, an unbounded version of the Möbius strip can be represented by the equation:
:<math>\log(r)\sin\left(\frac{1}{2}\theta\right)=z\cos\left(\frac{1}{2}\theta\right).</math>

=== Widest isometric embedding in 3-space ===
If a smooth Möbius strip in three-space is a rectangular one – that is, created from identifying two opposite sides of a geometrical rectangle with bending but not stretching the surface – then such an embedding is known to be possible if the aspect ratio of the rectangle is greater than the square root of three. (Note the shorter sides of the rectangle are identified to obtain the Möbius strip.) For an aspect ratio less than or equal to the square root of three, however, a smooth embedding of a rectangular Möbius strip into three-space may be impossible.

As the aspect ratio approaches the limiting ratio of {{sqrt|3}} from above, any such rectangular Möbius strip in three-space seems to approach a shape that in the limit can be thought of as a strip of three equilateral triangles, folded on top of one another so that they occupy just one equilateral triangle in three-space.

If the Möbius strip in three-space is only once continuously differentiable (in symbols: C<sup>1</sup>), however, then the theorem of Nash-Kuiper shows that no lower bound exists.

A method of making a Möbius strip from a rectangular strip too wide to simply twist and join (e.g., a rectangle only one unit long and one unit wide) is to first fold the wide direction back and forth using an even number of folds—an "accordion fold"—so that the folded strip becomes narrow enough that it can be twisted and joined, much as a single long-enough strip can be joined.<ref>{{cite book |last = Barr  |first = Stephen  |title = Experiments in Topology  |year = 1964 |publisher = Thomas Y. Crowell Company |location = New York |pages = 48,200–201 }}</ref> With two folds, for example, a {{nowrap|1 × 1}} strip would become a {{nowrap|1 × ⅓}} folded strip whose [[Cross section (geometry)|cross section]] is in the shape of an 'N' and would remain an 'N' after a half-twist. This folded strip, three times as long as it is wide, would be long enough to then join at the ends. This method works in principle, but becomes impractical after sufficiently many folds, if paper is used. Using normal paper, this construction can be [[Mathematics of paper folding#Flat folding|folded flat]], with all the layers of the paper in a single plane, but mathematically, whether this is possible without stretching the surface of the rectangle is not clear.<ref>Dmitry Fuchs and [[Serge Tabachnikov]], ''Mathematical Omnibus: Thirty Lectures on Classic Mathematics'', 2007, page 199, at http://www.math.psu.edu/tabachni/Books/taba.pdf</ref>

=== Topology ===
[[Topology|Topologically]], the Möbius strip can be defined as the [[square (geometry)|square]] <math>[0, 1] \times [0, 1]</math> with its top and bottom sides [[Quotient space (topology)|identified]] by the relation <math>(x, 0) \sim (1 - x, 1)</math> for <math>0 \le x \le 1</math>, as in the diagram on the right.

A less used presentation of the Möbius strip is as the topological quotient of a torus.<ref>Tony Phillips, ''[http://www.ams.org/mathmedia/archive/10-2006-media.html Tony Phillips' Take on Math in the Media],'' [[American Mathematical Society]], October 2006</ref> A torus can be constructed as the square <math>[0, 1] \times [0, 1]</math> with the edges identified as <math>(0, y) \sim (1, y)</math> (glue left to right) and <math>(x, 0) \sim (x, 1)</math> (glue bottom to top). If one then also identified {{nowrap|(''x'', ''y'') ~ (''y'', ''x'')}}, then one obtains the Möbius strip. The diagonal of the square (the points {{nowrap|(''x'', ''x'')}} where both coordinates agree) becomes the boundary of the Möbius strip, and carries an orbifold structure, which geometrically corresponds to "reflection" – [[geodesic]]s (straight lines) in the Möbius strip reflect off the edge back into the strip. Notationally, this is written as T<sup>2</sup>/S<sub>2</sub> – the 2-torus quotiented by the [[Group action (mathematics)|group action]] of the [[symmetric group]] on two letters (switching coordinates), and it can be thought of as the [[Configuration space (mathematics)|configuration space]] of two unordered points on the circle, possibly the same (the edge corresponds to the points being the same), with the torus corresponding to two ordered points on the circle.

The Möbius strip is a two-dimensional [[compact manifold]] (i.e. a [[Surface (topology)|surface]]) with boundary. It is a standard example of a surface that is not [[orientable manifold|orientable]]. In fact, the Möbius strip is the epitome of the topological phenomenon of [[Orientability|nonorientability]].  This is because two-dimensional shapes (surfaces) are the lowest-dimensional shapes for which nonorientability is possible and the Möbius strip is the '''only''' surface that is topologically a subspace of '''every''' nonorientable surface. As a result, any surface is nonorientable if and only if it contains a Möbius band as a subspace.

The Möbius strip is also a standard example used to illustrate the mathematical concept of a [[fiber bundle]]. Specifically, it is a nontrivial bundle over the circle ''S''<sup>1</sup> with a fiber the [[unit interval]], {{nowrap|1=''I'' = [0, 1]}}. Looking only at the edge of the Möbius strip gives a nontrivial two point (or '''Z'''<sub>2</sub><!-- What is Z2??-->) bundle over ''S''<sup>1</sup>.

=== Computer graphics ===
A simple construction of the Möbius strip that can be used to portray it in computer graphics or modeling packages is:
* Take a rectangular strip. Rotate it around a fixed point not in its plane. At every step, also rotate the strip along a line in its plane (the line that divides the strip in two) and perpendicular to the main orbital radius. The surface generated on one complete revolution is the Möbius strip.
* Take a Möbius strip and cut it along the middle of the strip.  This forms a new strip, which is a rectangle joined by rotating one end a whole turn.  By cutting it down the middle again, this forms two interlocking whole-turn strips.

=== Open Möbius band ===
The '''open Möbius band''' is formed by deleting the [[boundary (topology)|boundary]] of the standard Möbius band. It is constructed from the set {{nowrap|1=''S'' = { (''x'', ''y'') ∈ '''R'''<sup>2</sup> : 0 ≤ ''x'' ≤ 1 and 0 < ''y'' < 1 } }} by identifying (glueing) the points {{nowrap|(0, ''y'')}} and {{nowrap|(1, 1 − ''y'')}} for all {{nowrap|1=0 < ''y'' < 1}}.

It may be constructed as a surface of constant positive, negative, or zero (Gaussian) [[Gaussian curvature|curvature]]. In the cases of negative and zero curvature, the Möbius band can be constructed as a (geodesically) complete surface, which means that all geodesics ("straight lines" on the surface) may be extended indefinitely in either direction.

'''Constant negative curvature:'''
Like the plane and the open cylinder, the open Möbius band admits not only a complete metric of constant curvature 0, but also a complete metric of constant negative curvature, say −1.  One way to see this is to begin with the [[Poincaré half-plane model|upper half plane (Poincaré) model]] of the [[Hyperbolic geometry|hyperbolic plane]] ℍ, namely {{nowrap|1=ℍ = { (''x'', ''y'') ∈ ℝ<sup>2</sup> {{pipe}} ''y'' > 0} }} with the [[Riemannian metric]] given by {{nowrap|(''dx''<sup>2</sup> +  ''dy''<sup>2</sup>) / ''y''<sup>2</sup>}}.  The orientation-preserving isometries of this metric are all the maps {{nowrap|''f'' : ℍ → ℍ}} of the form {{nowrap|1=''f''(''z'') := (''az'' + ''b'') / (''cz'' + ''d'')}}, where ''a'', ''b'', ''c'', ''d'' are real numbers satisfying {{nowrap|1=''ad'' − ''bc'' = 1}}. Here ''z'' is a complex number with {{nowrap|Im(''z'') > 0}}, and we have identified ℍ with {{nowrap|{''z'' ∈ ℂ {{pipe}} Im(''z'') > 0} }} endowed with the Riemannian metric that was mentioned.  Then one orientation-reversing isometry ''g'' of ℍ given by {{nowrap|1=''g''(''z'') := -conj(''z'')}}, where conj(''z'') denotes the complex conjugate of ''z''.  These facts imply that the mapping {{nowrap|''h'' : ℍ → ℍ}} given by {{nowrap|1=''h''(''z'') := −2⋅conj(''z'')}} is an orientation-reversing isometry of ℍ that generates an infinite cyclic group ''G'' of isometries. (Its square is the isometry  {{nowrap|1=''h''(''z'') := 4⋅z}}, which can be expressed as {{nowrap|1=(''2z'' + ''0'') / (''0z'' + ''1/2'')}}.) The quotient {{nowrap|ℍ / ''G''}} of the action of this group can easily be seen to be topologically a Möbius band. But it is also easy to verify that it is complete and non-compact, with constant negative curvature −1.

The group of isometries of this Möbius band is 1-dimensional and is isomorphic to the special orthogonal group SO(2).

'''(Constant) zero curvature:'''
This may also be constructed as a complete surface, by starting with portion of the plane '''R'''<sup>2</sup> defined by {{nowrap|0 ≤ y ≤ 1}} and identifying {{nowrap|(''x'', 0)}} with {{nowrap|(−''x'', 1)}} for all ''x'' in '''R''' (the reals). The resulting metric makes the open Möbius band into a (geodesically) complete flat surface (i.e., having Gaussian curvature equal to 0 everywhere). This is the only metric on the Möbius band, up to uniform scaling, that is both flat and complete.

The group of isometries of this Möbius band is 1-dimensional and is isomorphic to the orthogonal group SO(2).

'''Constant positive curvature:'''
A Möbius band of constant positive curvature cannot be complete, since it is known that the only complete surfaces of constant positive curvature are the sphere and the [[Real projective plane|projective plane]].  The projective plane '''P'''<sup>2</sup> of constant curvature +1 may be constructed as the quotient of the unit sphere ''S''<sup>2</sup> in '''R'''<sup>3</sup> by the antipodal map ''A'': ''S''<sup>2</sup> → ''S''<sup>2</sup>, defined by {{nowrap|1=''A''(''x'', ''y'', ''z'') = (−''x'', −''y'', −''z'')}}.  The open Möbius band is homeomorphic to the once-punctured projective plane, that is, '''P'''<sup>2</sup> with any one point removed.  This may be thought of as the closest that a Möbius band of constant positive curvature can get to being a complete surface: just one point away.

The group of isometries of this Möbius band is also 1-dimensional and isomorphic to the orthogonal group O(2).

The space of unoriented lines in the plane is [[diffeomorphic]] to the open Möbius band.<ref>
{{cite journal|last=Parker|first=Phillip|year=1993|title=Spaces of Geodesics|journal=Aportaciones Matemáticas|series=Notas de Investigación|pages=67–79|url=http://www.math.wichita.edu/~pparker/research/sog.htm}}</ref> To see why, let ''L''(''θ'') denote the line through the origin at an angle ''θ'' to the positive x-axis.  For each ''L''(''θ'') there is the family ''P''(''θ'') of all lines in the plane that are perpendicular to ''L''(''θ'').  Topologically, the family ''P''(''θ'') is just a line (because each line in ''P''(''θ'') intersects the line ''L''(''θ'') in just one point).  In this way, as ''θ'' increases in the range {{nowrap|0° ≤ ''θ'' < 180°}}, the line ''L''(''θ'') represents a line's worth of distinct lines in the plane. But when ''θ'' reaches 180°, ''L''(180°) is identical to ''L''(0), and so the families ''P''(0°) and ''P''(180°) of perpendicular lines are also identical families.  The line ''L''(0°), however, has returned to itself as ''L''(180°) ''pointed in the opposite direction''. Every line in the plane corresponds to exactly one line in some family ''P''(''θ''), for exactly one ''θ'', for {{nowrap|0° ≤ ''θ'' < 180°}}, and ''P''(180°) is identical to ''P''(0°) but returns pointed in the opposite direction.  This ensures that the space of all lines in the plane – the union of all the ''L''(''θ'') for {{nowrap|0° ≤ ''θ'' ≤ 180°}} – is an open Möbius band.

The group of bijective linear transformations {{nowrap|GL(2, '''R''')}} of the plane to itself (real {{nowrap|2 × 2}} matrices with non-zero determinant) naturally induces bijections of '''the space of lines in the plane''' to itself, which form a group of self-homeomorphisms of the space of lines.  Hence the same group forms a group of self-homeomorphisms of the Möbius band described in the previous paragraph.  But there is no metric on the space of lines in the plane that is invariant under the action of this group of homeomorphisms. In this sense, the space of lines in the plane has no natural metric on it.

This means that the Möbius band possesses a natural 4-dimensional [[Lie group]] of self-homeomorphisms, given by {{nowrap|GL(2, '''R''')}}, but this high degree of symmetry cannot be exhibited as the group of isometries of any metric.

===Möbius band with round boundary===
The edge, or [[boundary (topology)|boundary]], of a Möbius strip is [[homeomorphic]] (topologically equivalent) to a [[circle]].  Under the usual embeddings of the strip in Euclidean space, as above, the boundary is not a true circle.  However, it is possible to [[embedding|embed]] a Möbius strip in three dimensions so that the boundary is a perfect circle lying in some plane.  For example, see Figures 307, 308, and 309 of "Geometry and the imagination".<ref>
{{cite book
  |author1=[[David Hilbert|Hilbert, David]] |author2=[[Stephan Cohn-Vossen|Cohn-Vossen, Stephan]]
 | title = Geometry and the Imagination   
  | edition = 2nd
  | year = 1952
  | publisher = Chelsea
  | isbn = 978-0-8284-1087-8}}
</ref>

A much more geometric embedding begins with a minimal [[Klein bottle]] immersed in the 3-sphere, as discovered by Blaine Lawson.  We then take half of this Klein bottle to get a Möbius band embedded in the 3-sphere (the unit sphere in 4-space). The result is sometimes called the "Sudanese Möbius Band"
,<ref>{{cite web
 |author1=Dan Asimov |author2=Doug Lerner | title = Issue 17 SIGGRAPH '84 Electronic Theater
 | year = 1984
 | url = http://www.siggraph.org/publications/video-review/1_36.php}}
</ref> where "sudanese" refers not to the country [[Sudan]] but to the names of two topologists, Sue Goodman and Daniel Asimov.  Applying stereographic projection to the Sudanese band places it in 3-dimensional space, as can be seen below – a version due to George Francis can be found [http://www.geom.uiuc.edu/graphics/pix/Special_Topics/Differential_Geometry/illiview.html here].

From Lawson's minimal Klein bottle we derive an embedding of the band into the [[3-sphere]] ''S''<sup>3</sup>, regarded as a subset of '''C'''<sup>2</sup>, which is geometrically the same as '''R'''<sup>4</sup>.  We map angles ''η'', ''φ'' to complex numbers ''z''<sub>1</sub>, ''z''<sub>2</sub> via
:<math>z_1 = \sin\eta\,e^{i\varphi}</math>
:<math>z_2 = \cos\eta\,e^{i\varphi/2}.</math>
Here the parameter ''η'' runs from 0 to ''π'' and ''φ'' runs from 0 to 2''π''. Since {{nowrap|1={{abs|&thinsp;''z''<sub>1</sub>&thinsp;}}<sup>2</sup> + {{abs|&thinsp;''z''<sub>2</sub>&thinsp;}}<sup>2</sup> = 1}}, the embedded surface lies entirely in ''S''<sup>3</sup>. The boundary of the strip is given by {{nowrap|1={{abs|&thinsp;''z''<sub>2</sub>&thinsp;}} = 1}} (corresponding to {{nowrap|1=''η'' = 0, ''π''}}), which is clearly a circle on the 3-sphere.

To obtain an embedding of the Möbius strip in '''R'''<sup>3</sup> one maps ''S''<sup>3</sup> to '''R'''<sup>3</sup> via a [[stereographic projection]]. The projection point can be any point on ''S''<sup>3</sup> that does not lie on the embedded Möbius strip (this rules out all the usual projection points). One possible choice is <math>\left\{1/\sqrt{2},i/\sqrt{2}\right\}</math>. Stereographic projections map circles to circles and preserves the circular boundary of the strip. The result is a smooth embedding of the Möbius strip into '''R'''<sup>3</sup> with a circular edge and no self-intersections.

[[File:MobiusSnail2B.png|center|580px]]

The Sudanese Möbius band in the three-sphere ''S''<sup>3</sup> is geometrically a fibre bundle over a great circle, whose fibres are great semicircles.  The most symmetrical image of a stereographic projection of this band into '''R'''<sup>3</sup> is obtained by using a projection point that lies on that great circle that runs through the midpoint of each of the semicircles. Each choice of such a projection point results in an image that is congruent to any other. But because such a projection point lies on the Möbius band itself, two aspects of the image are significantly different from the case (illustrated above) where the point is not on the band: 1) the image in '''R'''<sup>3</sup> is not the full Möbius band, but rather the band with one point removed (from its centerline); and 2) the image is unbounded – and as it gets increasingly far from the origin of '''R'''<sup>3</sup>, it increasingly approximates a plane.  Yet this version of the stereographic image has a group of 4 symmetries in '''R'''<sup>3</sup> (it is isomorphic to the [[Klein 4-group]]), as compared with the bounded version illustrated above having its group of symmetries the unique group of order 2. (If all symmetries and not just orientation-preserving isometries of '''R'''<sup>3</sup> are allowed, the numbers of symmetries in each case doubles.)

But the most geometrically symmetrical version of all is the original Sudanese Möbius band in the three-sphere ''S''<sup>3</sup>, where its full group of symmetries is isomorphic to the Lie group O(2). Having an infinite cardinality (that of the [[Continuum (set theory)|continuum]]), this is far larger than the symmetry group of any possible embedding of the Möbius band in '''R'''<sup>3</sup>.

==Related objects==
A closely related 'strange' geometrical object is the [[Klein bottle]]. A Klein bottle can be produced by gluing two Möbius strips together along their edges; this cannot be done in ordinary three-dimensional [[Euclidean space]] without creating self-intersections.<ref>
{{cite book
 | last = Spivak
 | first =  Michael
 | title = A Comprehensive Introduction to Differential Geometry, Volume I
 | edition = 2nd
 | series =
 | year =  1979
 | publisher = Publish or Perish
 | location = Wilmington, Delaware
 | pages = 591
 | chapter =
 | url =
 | quote =
 | ref =
 }}</ref>

Another closely related manifold is the [[real projective plane]]. If a circular disk is cut out of the real projective plane, what is left is a Möbius strip.<ref>
{{cite book
 | last1 = Hilbert
 | first1 =  David
 | last2 = Cohn-Vossen
 | first2 = S. 
 | edition = 2nd
 | title = Geometry and the Imagination
 | year =  1999
 | publisher = American Mathematical Society
 | location = Providence, Rhode Island
 | pages = 316
 | isbn = 978-0-8218-1998-2
 }}</ref> Going in the other direction, if one glues a disk to a Möbius strip by identifying their boundaries, the result is the projective plane. To visualize this, it is helpful to deform the Möbius strip so that its boundary is an ordinary circle (see above). The real projective plane, like the Klein bottle, cannot be embedded in three-dimensions without self-intersections.

In [[graph theory]], the [[Möbius ladder]] is a [[cubic graph]] closely related to the Möbius strip.

In 1968, Gonzalo Vélez Jahn (UCV, Caracas, Venezuela) discovered three dimensional bodies with Möbian characteristics;<ref>[http://demonstrations.wolfram.com/VelezJahnsMoebiusToroidalPolyhedron/ Wolfram Demonstration Project:  Vélez-Jahn's Möbius Toroidal Polyhedron]</ref> these were later described by [[Martin Gardner]] as prismatic rings that became toroidal polyhedrons in his August 1978 [[Mathematical Games column]] in Scientific American.<ref>This was the third time Gardner had featured the Möbius strip in his column.</ref>

==Applications==
[[File:Moebiusstripscarf.jpg|right|thumb|200px|[[Mathematics and art|Mathematical art]]: a [[scarf]] designed as a Möbius strip]]
There have been several technical applications for the Möbius strip.  Giant Möbius strips have been used as [[conveyor belt]]s that last longer because the entire surface area of the belt gets the same amount of wear, and as continuous-loop recording tapes (to double the playing time).  Möbius strips are common in the manufacture of fabric computer printer and [[typewriter ribbon]]s, as they let the ribbon be twice as wide as the print head while using both halves evenly.<ref>Hogarth, Ian W. and Kiewning, Friedhelm. (1991) "Typewriter or printer ribbon and method for its manufacture" {{US Patent|5062725}}</ref>

A [[Möbius resistor]] is an electronic circuit element that cancels its own inductive reactance. [[Nikola Tesla]] patented similar technology in 1894:<ref>Tesla, Nikola (1894) "Coil for Electro-Magnets" {{US Patent|512340}}</ref> "Coil for Electro Magnets" was intended for use with his system of global transmission of electricity without wires.

The Möbius strip is the [[Configuration space (mathematics)|configuration space]] of two unordered points on a circle.  Consequently, in [[music theory]], the space of all two-note chords, known as [[Dyad (music)|dyads]], takes the shape of a Möbius strip; this and generalizations to more points is a significant [[Orbifold#Music theory|application of orbifolds to music theory]].<ref>[http://www.livescience.com/strangenews/080507-math-music.html Clara Moskowitz, Music Reduced to Beautiful Math, LiveScience]</ref><ref>{{cite journal |author= Dmitri Tymoczko |title= The Geometry of Musical Chords |date= 7 July 2006 |volume= 313 |issue= 5783 |pages= 72–4 |journal= [[Science (journal)|Science]] |doi= 10.1126/science.1126287 |pmid= 16825563|bibcode= 2006Sci...313...72T |citeseerx= 10.1.1.215.7449 }}</ref>

In [[physics]]/electro-technology as:
* A compact resonator with a resonance frequency that is half that of identically constructed linear coils<ref>{{cite journal|doi=10.1109/22.898999|title=Mobius dual-mode resonators and bandpass filters|journal=IEEE Transactions on Microwave Theory and Techniques|volume=48|issue=12|pages=2465–2471|year=2000|last1=Pond|first1=J.M.|bibcode=2000ITMTT..48.2465P}}</ref>
* An inductionless resistor<ref>Davis, Richard L (1966) "Non-inductive electrical resistor" {{US patent|3267406}}</ref>
* [[Superconductors]] with high transition temperature<ref>{{Cite journal|first=Raul Perez|last=Enriquez|title=A Structural parameter for High Tc Superconductivity from an Octahedral Moebius Strip in RBaCuO: 123 type of perovskite|journal=Rev Mex Fis|volume=48|issue=supplement 1|year=2002|page=262|arxiv=cond-mat/0308019|bibcode=2003cond.mat..8019P}}</ref>
* Möbius resonator <ref>{{cite journal|title=Printed Resonators: Mobius Strip Theory and Applications|journal=Microwave Journal|volume=56|issue=11|date=November 2013| url=https://synergymwave.com/articles/2013/11/article.pdf}} </ref>

In [[chemistry]]/nano-technology as:
* [[Molecular knot]]s with special characteristics (Knotane [2], Chirality)
* Molecular engines<ref>{{cite journal|pmid=15704147|year=2005|author1=Lukin|first1=O|title=Knotting and threading of molecules: Chemistry and chirality of molecular knots and their assemblies|journal=Angewandte Chemie International Edition|volume=44|issue=10|pages=1456–77|last2=Vögtle|first2=F|doi=10.1002/anie.200460312}}</ref>
* Graphene volume (nano-graphite) with new electronic characteristics, like helical magnetism<ref>{{Cite journal|title=Novel Electronic States in Graphene Ribbons -Competing Spin and Charge Orders-|first1=Atsushi|last1=Yamashiro|first2=Yukihiro|last2=Shimoi|first3=Kikuo|last3=Harigaya|first4=Katsunori|last4=Wakabayashi|arxiv=cond-mat/0309636|journal=Physica E|volume=22|issue=1–3|pages=688–691|year=2004|doi=10.1016/j.physe.2003.12.100|bibcode=2004PhyE...22..688Y}}</ref>
* A special type of aromaticity: [[Möbius aromaticity]]
* Charged particles caught in the magnetic field of the earth that can move on a Möbius band
*The [[cyclotide]] (cyclic protein) kalata B1, active substance of the plant ''Oldenlandia affinis'', contains Möbius topology for the peptide backbone.

=== In stage magic ===
The Möbius strip principle has been used as a method of creating [[Magic (illusion)|the illusion of magic]]. The trick, known as the Afghan bands, was very popular in the first half of the twentieth century. Many versions of this trick exist and have been performed by famous illusionists such as [[Harry Blackstone Sr.]] and [[Thomas Nelson Downs]].<ref>{{Cite book|url=https://magicperspectives.net/afghan-bands/|title=The Möbius Strip in Magic: A Treatise on the Afghan Bands|last=Prevos|first=Peter|publisher=Third Hemisphere|year=2018|isbn=|location=Kangaroo Flat|pages=}}</ref><ref>{{Cite book|title=Mathematics, Magic and Mystery|last=Gardner|first=Martin|publisher=Dover Books|year=1956|isbn=|location=New York|pages=70–73}}</ref>

==See also==
*[[Cross-cap]]
*[[Umbilic torus]]
* [[Ribbon theory]]

==References==
{{Reflist|30em}}

==External links==
{{Wiktionary|Möbius strip}}
{{Commons category|Moebius strip|Möbius strip}}
*[http://mechproto.olin.edu/final_projects/average_jo.html The Möbius Gear – A functional planetary gear model in which one gear is a Möbius strip]
*{{MathWorld|urlname=MoebiusStrip|title=Möbius Strip}}

{{DEFAULTSORT:Mobius Strip}}
[[:Category:Topology]]
[[:Category:Recreational mathematics]]
[[:Category:Surfaces]]