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==Examples== ===Surfaces=== The Euler characteristic can be calculated easily for general surfaces by finding a polygonization of the surface (that is, a description as a [[CW-complex]]) and using the above definitions. {| class="wikitable" |- !Name !Image !<abbr title="Euler characteristic">'''χ'''</abbr> |- |[[Interval (mathematics)|Interval]] |[[Image:Complete graph K2.svg|100px]] |'''{{0}}1''' |- |[[Circle]] |[[Image:Cirklo.svg|100px]] |'''{{0}}0''' |- |[[Unit disk|Disk]] |[[Image:Disc Plain grey.svg|100px]] |'''{{0}}1''' |- |[[Sphere]] |[[Image:Sphere-wireframe.png|100px]] |'''{{0}}2''' |- |[[Torus]] <br>''(Product of<br>two circles)'' |[[Image:Torus illustration.png|100px]] |'''{{0}}0''' |- |[[Double torus]] |[[Image:Double torus illustration.png|100px]] |'''−2''' |- |[[Triple torus]] |[[Image:Triple torus illustration.png|100px]] |'''−4''' |- |[[Real projective plane|Real projective<br>plane]] |[[Image:Steiners Roman.png|100px]] |'''{{0}}1''' |- |[[Möbius strip]] |[[Image:MobiusStrip-01.svg|100px]] |'''{{0}}0''' |- |[[Klein bottle]] |[[Image:KleinBottle-01.png|100px]] |'''{{0}}0''' |- |Two spheres<br>(not connected) <br>''(Disjoint union<br>of two spheres)'' |[[File:2-spheres.png|200x200px]] |2 + 2 = '''4''' |- |Three spheres<br>(not connected) <br>''(Disjoint union<br>of three spheres)'' |[[File:Sphere-wireframe.png|100x100px]][[File:Sphere-wireframe.png|100x100px]][[File:Sphere-wireframe.png|100x100px]] |2 + 2 + 2 = '''6''' |- |<math>n</math> spheres<br>(not connected) <br>''(Disjoint union<br>of ''n'' spheres)'' | [[File:Sphere-wireframe.png|100x100px]]'''<big> ...</big>'''[[File:Sphere-wireframe.png|100x100px]] |{{nowrap|2 + ... + 2 {{=}} '''2n'''}} |} ===Soccer ball=== It is common to construct [[soccer ball]]s by stitching together pentagonal and hexagonal pieces, with three pieces meeting at each vertex (see for example the [[Adidas Telstar]]). If {{mvar|P}} pentagons and {{mvar|H}} hexagons are used, then there are <math>\ F = P + H\ </math> faces, <math>\ V = \tfrac{1}{3}\left(\ 5 P + 6 H\ \right)\ </math> vertices, and <math>\ E = \tfrac{1}{2} \left(\ 5P + 6H\ \right)\ </math> edges. The Euler characteristic is thus : <math> V - E + F = \tfrac{1}{3} \left(\ 5 P + 6 H\ \right) - \tfrac{1}{2} \left(\ 5 P + 6 H\ \right) + P + H = \tfrac{1}{6} P ~.</math> Because the sphere has Euler characteristic 2, it follows that <math>\ P = 12 ~.</math> That is, a soccer ball constructed in this way always has 12 pentagons. The number of hexagons can be any [[nonnegative integer]] except 1.<ref>{{cite book |first1=P.W. |last1=Fowler |name-list-style=amp |first2=D.E. |last2=Manolopoulos |year=1995 |title=An Atlas of Fullerenes |page=32}}</ref> This result is applicable to [[fullerene]]s and [[Goldberg polyhedra]]. ===Arbitrary dimensions=== [[File:Euler_characteristic_hypercube_simplex.svg|thumb|250px|Comparison of Euler characteristics of [[hypercube]]s and [[simplex|simplices]] of dimensions 1 to 4]] {| class="wikitable floatright" style="text-align:right;" |+ <small>Euler characteristics of the six [[regular 4-polytope|4 dimensional analogues of the regular polyhedra]]</small> ! Regular<br/>4 polytope ! [[Vertex (geometry)|{{mvar|V}}]]<br/>{{mvar|k}}{{sub|0}} ! [[Edge (geometry)|{{mvar|E}}]]<br/>{{mvar|k}}{{sub|1}} ! [[Face (geometry)|{{mvar|F}}]]<br/>{{mvar|k}}{{sub|2}} ! [[Cell (geometry)|{{mvar|C}}]]<br/>{{mvar|k}}{{sub|3}} ! {{right| <math> \chi = V - E\ +</math><br/><math> +\ F - C</math>}} |- | [[5-cell|5 cell]] || 5 || 10 || 10 || 5 || {{center|'''0'''}} |- | [[8-cell|8 cell]] || 16 || 32 || 24 || 8 || {{center|'''0'''}} |- | [[16-cell|16 cell]] || 8 || 24 || 32 || 16 || {{center|'''0'''}} |- | [[24-cell|24 cell]] || 24 || 96 || 96 || 24 || {{center|'''0'''}} |- | [[120-cell|120 cell]] || 600 || 1200 || 720 || 120 || {{center|'''0'''}} |- | [[600-cell|600 cell]] || 120 || 720 || 1200 || 600 || {{center|'''0'''}} |} The {{mvar|n}} dimensional sphere has singular [[homology group]]s equal to :<math>H_k(\mathrm{S}^n) = \begin{cases} \mathbb{Z} ~& k = 0 ~~ \mathsf{ or } ~~ k = n \\ \{0\} & \mathsf{otherwise}\ , \end{cases}</math> hence has Betti number 1 in dimensions 0 and {{mvar|n}}, and all other Betti numbers are 0. Its Euler characteristic is then {{nobr|{{math|χ {{=}} 1 + (−1)}}{{sup| {{mvar|n}} }} ;}} that is, either 0 if {{mvar|n}} is [[odd number|odd]], or 2 if {{mvar|n}} is [[even number|even]]. The {{mvar|n}} dimensional real [[projective space]] is the quotient of the {{mvar|n}} sphere by the [[antipodal map]]. It follows that its Euler characteristic is exactly half that of the corresponding sphere – either 0 or 1. The {{mvar|n}} dimensional torus is the product space of {{mvar|n}} circles. Its Euler characteristic is 0, by the product property. More generally, any compact [[parallelizable manifold]], including any compact [[Lie group]], has Euler characteristic 0.<ref>{{cite book |author1-link=John Milnor |last1=Milnor |first1=J.W. |name-list-style=amp |last2=Stasheff |first2=James D. |year=1974 |title=Characteristic Classes |publisher=Princeton University Press}}</ref> The Euler characteristic of any [[closed manifold|closed]] odd-dimensional manifold is also 0.<ref>{{harvp|Richeson|2008|p=261}}</ref> The case for [[Orientability|orientable]] examples is a corollary of [[Poincaré duality]]. This property applies more generally to any [[compact space|compact]] [[topologically stratified space|stratified space]] all of whose strata have odd dimension. It also applies to closed odd-dimensional non-orientable manifolds, via the two-to-one [[Orientability#Orientable double cover|orientable double cover]].
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