Antiprism

Set of uniform $n$ -gonal antiprisms
Set of uniform n-gonal antiprisms
	Uniform hexagonal antiprism (n = 6)
Type	uniform in the sense of semiregular polyhedron
Faces	2 regular n-gons; 2n equilateral triangles
Edges	4n
Vertices	2n
Vertex configuration	3.3.3.n
Schläfli symbol	{ }⊗{n} ; s{2,2n}; sr{2,n}
Conway notation	An
Coxeter diagram	;
Symmetry group	Dnd, [2+,2n], (2*n), order 4n
Rotation group	Dn, [2,n]+, (22n), order 2n
Dual polyhedron	convex dual-uniform n-gonal trapezohedron
Properties	convex, vertex-transitive, regular polygon faces, congruent & coaxial bases
Net
	Net of uniform enneagonal antiprism (n = 9)

In geometry, an $n$ -gonal antiprism or $n$ -antiprism is a polyhedron composed of two parallel direct copies (not mirror images) of an $n$ -sided polygon, connected by an alternating band of $2 n$ triangles. They are represented by the Conway notation $A n$ .

Antiprisms are a subclass of prismatoids, and are a (degenerate) type of snub polyhedron.

Antiprisms are similar to prisms, except that the bases are twisted relatively to each other, and that the side faces (connecting the bases) are $2 n$ triangles, rather than $n$ quadrilaterals.

The dual polyhedron of an $n$ -gonal antiprism is an $n$ -gonal trapezohedron.

History

At the intersection of modern-day graph theory and coding theory, the triangulation of a set of points have interested mathematicians since Isaac Newton, who fruitlessly sought a mathematical proof of the kissing number problem in 1694.^[2] The existence of antiprisms was discussed, and their name was coined by Johannes Kepler, though it is possible that they were previously known to Archimedes, as they satisfy the same conditions on faces and on vertices as the Archimedean solids.^{[citation needed]} According to Ericson and Zinoviev, Harold Scott MacDonald Coxeter wrote at length on the topic,^[2] and was among the first to apply the mathematics of Victor Schlegel to this field.

Knowledge in this field is "quite incomplete" and "was obtained fairly recently", i.e. in the 20th century^{[citation needed]}. For example, as of 2001 it had been proven for only a limited number of non-trivial cases that the $n$ -gonal antiprism is the mathematically optimal arrangement of $2 n$ points in the sense of maximizing the minimum Euclidean distance between any two points on the set: in 1943 by László Fejes Tóth for 4 and 6 points (digonal and trigonal antiprisms, which are Platonic solids); in 1951 by Kurt Schütte and Bartel Leendert van der Waerden for 8 points (tetragonal antiprism, which is not a cube).^[2]

The chemical structure of binary compounds has been remarked to be in the family of antiprisms;^[3] especially those of the family of boron hydrides (in 1975) and carboranes because they are isoelectronic. This is a mathematically real conclusion reached by studies of X-ray diffraction patterns,^[4] and stems from the 1971 work of Kenneth Wade,^[5] the nominative source for Wade's rules of polyhedral skeletal electron pair theory.

Rare-earth metals such as the lanthanides form antiprismatic compounds with some of the halides or some of the iodides. The study of crystallography is useful here.^[6] Some lanthanides, when arranged in peculiar antiprismatic structures with chlorine and water, can form molecule-based magnets.^[7]

Right antiprism

For an antiprism with regular $n$ -gon bases, one usually considers the case where these two copies are twisted by an angle of $.mw-parser-output .sfrac{white-space:nowrap}.mw-parser-output .sfrac.tion,.mw-parser-output .sfrac .tion{display:inline-block;vertical-align:-0.5em;font-size:85%;text-align:center}.mw-parser-output .sfrac .num,.mw-parser-output .sfrac .den{display:block;line-height:1em;margin:0 0.1em}.mw-parser-output .sfrac .den{border-top:1px solid}.mw-parser-output .sr-only{border:0;clip:rect(0,0,0,0);height:1px;margin:-1px;overflow:hidden;padding:0;position:absolute;width:1px}180/n$ degrees.

The axis of a regular polygon is the line perpendicular to the polygon plane and lying in the polygon centre.

For an antiprism with congruent regular $n$ -gon bases, twisted by an angle of $180 / n$ degrees, more regularity is obtained if the bases have the same axis: are coaxial; i.e. (for non-coplanar bases): if the line connecting the base centers is perpendicular to the base planes. Then the antiprism is called a right antiprism, and its $2 n$ side faces are isosceles triangles.

Uniform antiprism

A uniform $n$ -antiprism has two congruent regular $n$ -gons as base faces, and $2 n$ equilateral triangles as side faces.

Uniform antiprisms form an infinite class of vertex-transitive polyhedra, as do uniform prisms. For $n = 2$ , we have the regular tetrahedron as a digonal antiprism (degenerate antiprism); for $n = 3$ , the regular octahedron as a triangular antiprism (non-degenerate antiprism).

Family of uniform n-gonal antiprisms
v
t
e
Antiprism name	Digonal antiprism	(Trigonal) Triangular antiprism	(Tetragonal) Square antiprism	Pentagonal antiprism	Hexagonal antiprism	Heptagonal antiprism	Octagonal antiprism	Enneagonal antiprism	Decagonal antiprism	Hendecagonal antiprism	Dodecagonal antiprism	...	Apeirogonal antiprism
Polyhedron image												...
Spherical tiling image												Plane tiling image
Vertex config.	2.3.3.3	3.3.3.3	4.3.3.3	5.3.3.3	6.3.3.3	7.3.3.3	8.3.3.3	9.3.3.3	10.3.3.3	11.3.3.3	12.3.3.3	...	∞.3.3.3

Schlegel diagrams

A3	A4	A5	A6	A7	A8

Cartesian coordinates

Cartesian coordinates for the vertices of a right $n$ -antiprism (i.e. with regular $n$ -gon bases and $2 n$ isosceles triangle side faces) are:

\left(\cos {\frac {k\pi }{n}},\sin {\frac {k\pi }{n}},(-1)^{k}h\right)

where $0 \leq k \leq 2 n - 1$ ;

if the $n$ -antiprism is uniform (i.e. if the triangles are equilateral), then:

2h^{2}=\cos {\frac {\pi }{n}}-\cos {\frac {2\pi }{n}}.

Volume and surface area

Let $a$ be the edge-length of a uniform $n$ -gonal antiprism; then the volume is:

V={\frac {n~{\sqrt {4\cos ^{2}{\frac {\pi }{2n}}-1}}\sin {\frac {3\pi }{2n}}}{12\sin ^{2}{\frac {\pi }{n}}}}~a^{3},

and the surface area is:

A={\frac {n}{2}}\left(\cot {\frac {\pi }{n}}+{\sqrt {3}}\right)a^{2}.

Related polyhedra

There are an infinite set of truncated antiprisms, including a lower-symmetry form of the truncated octahedron (truncated triangular antiprism). These can be alternated to create snub antiprisms, two of which are Johnson solids, and the snub triangular antiprism is a lower symmetry form of the regular icosahedron.

Antiprisms
				...
s{2,4}	s{2,6}	s{2,8}	s{2,10}	s{2,2n}
Truncated antiprisms
				...
ts{2,4}	ts{2,6}	ts{2,8}	ts{2,10}	ts{2,2n}
Snub antiprisms
J₈₄	Icosahedron	J₈₅	Irregular faces...
				...
ss{2,4}	ss{2,6}	ss{2,8}	ss{2,10}	ss{2,2n}

Symmetry

The symmetry group of a right $n$ -antiprism (i.e. with regular bases and isosceles side faces) is $D n d = D n v$ of order $4 n$ , except in the cases of:

$n = 2$ : the regular tetrahedron, which has the larger symmetry group $T d$ of order $24 = 3\times(4\times2)$ , which has three versions of $D 2d$ as subgroups;

$n = 3$ : the regular octahedron, which has the larger symmetry group $O h$ of order $48 = 4\times(4\times3)$ , which has four versions of $D 3d$ as subgroups.

The symmetry group contains inversion if and only if $n$ is odd.

The rotation group is $D n$ of order $2 n$ , except in the cases of:

$n = 2$ : the regular tetrahedron, which has the larger rotation group $T$ of order $12 = 3\times(2\times2)$ , which has three versions of $D 2$ as subgroups;

$n = 3$ : the regular octahedron, which has the larger rotation group $O$ of order $24 = 4\times(2\times3)$ , which has four versions of $D 3$ as subgroups.

Note: The right $n$ -antiprisms have congruent regular $n$ -gon bases and congruent isosceles triangle side faces, thus have the same (dihedral) symmetry group as the uniform $n$ -antiprism, for $n \geq 4$ .

Star antiprism

5/2-antiprism			5/3-antiprism
9/2-antiprism		9/4-antiprism		9/5-antiprism

This shows all the non-star and star antiprisms up to 15 sides, together with those of a 29-gon.

Uniform star antiprisms are named by their star polygon bases, {p/q}, and exist in prograde and in retrograde (crossed) solutions. Crossed forms have intersecting vertex figures, and are denoted by "inverted" fractions: p/(p – q) instead of p/q; example: 5/3 instead of 5/2.

A right star antiprism has two congruent coaxial regular convex or star polygon base faces, and 2n isosceles triangle side faces.

Any star antiprism with regular convex or star polygon bases can be made a right star antiprism (by translating and/or twisting one of its bases, if necessary).

In the retrograde forms but not in the prograde forms, the triangles joining the convex or star bases intersect the axis of rotational symmetry. Thus:

Retrograde star antiprisms with regular convex polygon bases cannot have all equal edge lengths, so cannot be uniform. "Exception": a retrograde star antiprism with equilateral triangle bases (vertex configuration: 3.3/2.3.3) can be uniform; but then, it has the appearance of an equilateral triangle: it is a degenerate star polyhedron.

Similarly, some retrograde star antiprisms with regular star polygon bases cannot have all equal edge lengths, so cannot be uniform. Example: a retrograde star antiprism with regular star 7/5-gon bases (vertex configuration: 3.3.3.7/5) cannot be uniform.

Also, star antiprism compounds with regular star p/q-gon bases can be constructed if p and q have common factors. Example: a star 10/4-antiprism is the compound of two star 5/2-antiprisms.

Star p/q-antiprisms by symmetry, for p ≤ 12
Symmetry group	Uniform stars			Right stars
D_4d [2⁺,8] (2*4)				3.3/2.3.4
D_5h [2,5] (*225)	3.3.3.5/2			3.3/2.3.5
D_5d [2⁺,10] (2*5)	3.3.3.5/3
D_6d [2⁺,12] (2*6)				3.3/2.3.6
D_7h [2,7] (*227)	3.3.3.7/2	3.3.3.7/4
D_7d [2⁺,14] (2*7)	3.3.3.7/3
D_8d [2⁺,16] (2*8)	3.3.3.8/3	3.3.3.8/5
D_9h [2,9] (*229)	3.3.3.9/2	3.3.3.9/4
D_9d [2⁺,18] (2*9)	3.3.3.9/5
D_10d [2⁺,20] (2*10)	3.3.3.10/3
D_11h [2,11] (*2.2.11)	3.3.3.11/2	3.3.3.11/4	3.3.3.11/6
D_11d [2⁺,22] (2*11)	3.3.3.11/3	3.3.3.11/5	3.3.3.11/7
D_12d [2⁺,24] (2*12)	3.3.3.12/5	3.3.3.12/7
...	...

References

^ N.W. Johnson: Geometries and Transformations, (2018) ISBN 978-1-107-10340-5 Chapter 11: Finite symmetry groups, 11.3 Pyramids, Prisms, and Antiprisms, Figure 11.3c
^ ^a ^b ^c Ericson, Thomas; Zinoviev, Victor (2001). "Codes in dimension n = 3". Codes on Euclidean Spheres. North-Holland Mathematical Library. Vol. 63. pp. 67–106. doi:10.1016/S0924-6509(01)80048-9. ISBN 9780444503299.
^ Beall, Herbert; Gaines, Donald F. (2003). "Boron Hydrides". Encyclopedia of Physical Science and Technology. pp. 301–316. doi:10.1016/B0-12-227410-5/00073-9. ISBN 9780122274107.
^ “Boron Hydride Chemistry” (E. L. Muetterties, ed.), Academic Press, New York
^ Wade, K. (1971). "The structural significance of the number of skeletal bonding electron-pairs in carboranes, the higher boranes and borane anions, and various transition-metal carbonyl cluster compounds". J. Chem. Soc. D. 1971 (15): 792–793. doi:10.1039/C29710000792.
^ Meyer, Gerd (2014). [10.1016/B978-0-444-63256-2.00264-3 "Symbiosis of Intermetallic and Salt"]. Including Actinides. Handbook on the Physics and Chemistry of Rare Earths. Vol. 45. pp. 111–178. doi:10.1016/B978-0-444-63256-2.00264-3. ISBN 9780444632562. {{cite book}}: Check |chapter-url= value (help)
^ Bartolomé, Elena; Arauzo, Ana; Luzón, Javier; Bartolomé, Juan; Bartolomé, Fernando (2017). Magnetic Relaxation of Lanthanide-Based Molecular Magnets. Handbook of Magnetic Materials. Vol. 26. pp. 1–289. doi:10.1016/bs.hmm.2017.09.002. ISBN 9780444639271.

Bibliography

Anthony Pugh (1976). Polyhedra: A visual approach. California: University of California Press Berkeley. ISBN 0-520-03056-7. Chapter 2: Archimedean polyhedra, prisms and antiprisms

External links

Media related to Antiprism at Wikimedia Commons
Weisstein, Eric W. "Antiprism". MathWorld.
Nonconvex Prisms and Antiprisms
Paper models of prisms and antiprisms

[1] N.W. Johnson: Geometries and Transformations, (2018) ISBN 978-1-107-10340-5 Chapter 11: Finite symmetry groups, 11.3 Pyramids, Prisms, and Antiprisms, Figure 11.3c

[ericson01-2] Ericson, Thomas; Zinoviev, Victor (2001). "Codes in dimension n = 3". Codes on Euclidean Spheres. North-Holland Mathematical Library. Vol. 63. pp. 67–106. doi:10.1016/S0924-6509(01)80048-9. ISBN 9780444503299.

[beall03-3] Beall, Herbert; Gaines, Donald F. (2003). "Boron Hydrides". Encyclopedia of Physical Science and Technology. pp. 301–316. doi:10.1016/B0-12-227410-5/00073-9. ISBN 9780122274107.

[muetterties75-4] “Boron Hydride Chemistry” (E. L. Muetterties, ed.), Academic Press, New York

[wade71-5] Wade, K. (1971). "The structural significance of the number of skeletal bonding electron-pairs in carboranes, the higher boranes and borane anions, and various transition-metal carbonyl cluster compounds". J. Chem. Soc. D. 1971 (15): 792–793. doi:10.1039/C29710000792.

[meyer11-6] Meyer, Gerd (2014). [10.1016/B978-0-444-63256-2.00264-3 "Symbiosis of Intermetallic and Salt"]. Including Actinides. Handbook on the Physics and Chemistry of Rare Earths. Vol. 45. pp. 111–178. doi:10.1016/B978-0-444-63256-2.00264-3. ISBN 9780444632562. {{cite book}}: Check |chapter-url= value (help)

[bartolome17-7] Bartolomé, Elena; Arauzo, Ana; Luzón, Javier; Bartolomé, Juan; Bartolomé, Fernando (2017). Magnetic Relaxation of Lanthanide-Based Molecular Magnets. Handbook of Magnetic Materials. Vol. 26. pp. 1–289. doi:10.1016/bs.hmm.2017.09.002. ISBN 9780444639271.

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