Platonic solid

In geometry, a Platonic solid is a convex, regular polyhedron in three-dimensional Euclidean space. Being a regular polyhedron means that the faces are congruent (identical in shape and size) regular polygons (all angles congruent and all edges congruent), and the same number of faces meet at each vertex. There are only five such polyhedra: a tetrahedron (four triangular faces), a cube (six square faces), an octahedron (eight triangular faces), a dodecahedron (twelve pentagonal faces), and an icosahedron (twenty triangular faces).

Geometers have studied the Platonic solids for thousands of years.^[1] They are named for the ancient Greek philosopher Plato, who hypothesized in one of his dialogues, the Timaeus, that the classical elements were made of these regular solids.^[2]

The Platonic solids have been known since antiquity. It has been suggested that certain carved stone balls created by the late Neolithic people of Scotland represent these shapes. However, these balls have rounded knobs rather than being polyhedral. The number of knobs frequently differed from the numbers of vertices of the Platonic solids. No ball whose knobs match the 20 vertices of the dodecahedron, and the arrangement of the knobs was not always symmetrical.^[3]

The ancient Greeks studied the Platonic solids extensively. Some sources (such as Proclus) credit Pythagoras with their discovery. Other evidence suggests that he may have only been familiar with the tetrahedron, cube, and dodecahedron and that the discovery of the octahedron and icosahedron belong to Theaetetus, a contemporary of Plato. In any case, Theaetetus gave a mathematical description of all five and may have been responsible for the first known proof that no other convex regular polyhedra exist.

The Platonic solids are prominent in the philosophy of Plato, their namesake. Plato wrote about them in the dialogue Timaeus c. 360 B.C. in which he associated each of the four classical elements (earth, air, water, and fire) with a regular solid. Earth was associated with the cube, air with the octahedron, water with the icosahedron, and fire with the tetrahedron. Of the fifth Platonic solid, the dodecahedron, Plato obscurely remarked, "...the god used [it] for arranging the constellations on the whole heaven". Aristotle added a fifth element, aither (aether in Latin, "ether" in English) and postulated that the heavens were made of this element, but he had no interest in matching it with Plato's fifth solid.^[5]

Euclid completely mathematically described the Platonic solids in the Elements, the last book (Book XIII) of which is devoted to their properties. Propositions 13–17 in Book XIII describe the construction of the tetrahedron, octahedron, cube, icosahedron, and dodecahedron in that order. For each solid, Euclid finds the ratio of the diameter of the circumscribed sphere to the edge length. In Proposition 18 he argues that there are no further convex regular polyhedra. Andreas Speiser has advocated the view that the construction of the five regular solids is the chief goal of the deductive system canonized in the Elements.^[6] Much of the information in Book XIII is probably derived from the work of Theaetetus.

In the 16th century, the German astronomer Johannes Kepler attempted to relate the five extraterrestrial planets known at that time to the five Platonic solids. In Mysterium Cosmographicum, published in 1596, Kepler proposed a model of the Solar System in which the five solids were set inside one another and separated by a series of inscribed and circumscribed spheres. Kepler proposed that the distance relationships between the six planets known at that time could be understood in terms of the five Platonic solids enclosed within a sphere that represented the orbit of Saturn. The six spheres each corresponded to one of the planets (Mercury, Venus, Earth, Mars, Jupiter, and Saturn). The solids were ordered with the innermost being the octahedron, followed by the icosahedron, dodecahedron, tetrahedron, and finally the cube, thereby dictating the structure of the solar system and the distance relationships between the planets by the Platonic solids. In the end, Kepler's original idea had to be abandoned, but out of his research came his three laws of orbital dynamics, the first of which was that the orbits of planets are ellipses rather than circles, changing the course of physics and astronomy.^[7] He also discovered the Kepler solids, which are two nonconvex regular polyhedra.

For Platonic solids centered at the origin, simple Cartesian coordinates of the vertices are given below. The Greek letter φ {\displaystyle \varphi } is used to represent the golden ratio 1 + 5 2 ≈ 1.6180 {\displaystyle {\frac {1+{\sqrt {5}}}{2}}\approx 1.6180} .

Parameters

Figure	Tetrahedron		Octahedron	Cube	Icosahedron		Dodecahedron
Faces	4		8	6	20		12
Vertices	4		6 (2 × 3)	8	12 (4 × 3)		20 (8 + 4 × 3)
Position	1	2			1	2	1	2
Vertex coordinates	(1, 1, 1) (1, −1, −1) (−1, 1, −1) (−1, −1,  1)	(−1, −1, −1) (−1, 1, 1) ( 1, −1,  1) ( 1,  1, −1)	(±1,  0,  0) ( 0, ±1,  0) ( 0,  0, ±1)	(±1, ±1, ±1)	( 0, ±1, ±φ) (±1, ±φ,  0) (±φ,  0, ±1)	( 0, ±φ, ±1) (±φ, ±1,  0) (±1,  0, ±φ)	(±1, ±1, ±1) ( 0, ±⁠1/φ⁠, ±φ) (±⁠1/φ⁠, ±φ,  0) (±φ,  0, ±⁠1/φ⁠)	(±1, ±1, ±1) ( 0, ±φ, ±⁠1/φ⁠) (±φ, ±⁠1/φ⁠,  0) (±⁠1/φ⁠,  0, ±φ)

The coordinates for the tetrahedron, dodecahedron, and icosahedron are given in two positions such that each can be deduced from the other: in the case of the tetrahedron, by changing all coordinates of sign (central symmetry), or, in the other cases, by exchanging two coordinates (reflection with respect to any of the three diagonal planes).

These coordinates reveal certain relationships between the Platonic solids: the vertices of the tetrahedron represent half of those of the cube, as {4,3} or , one of two sets of 4 vertices in dual positions, as h{4,3} or . Both tetrahedral positions make the compound stellated octahedron.

The coordinates of the icosahedron are related to two alternated sets of coordinates of a nonuniform truncated octahedron, t{3,4} or , also called a snub octahedron, as s{3,4} or , and seen in the compound of two icosahedra.

Eight of the vertices of the dodecahedron are shared with the cube. Completing all orientations leads to the compound of five cubes.

A convex polyhedron is a Platonic solid if and only if all three of the following requirements are met.

• All of its faces are congruent convex regular polygons.
• None of its faces intersect except at their edges.
• The same number of faces meet at each of its vertices.

Each Platonic solid can therefore be assigned a pair {p, q} of integers, where p is the number of edges (or, equivalently, vertices) of each face, and q is the number of faces (or, equivalently, edges) that meet at each vertex. This pair {p, q}, called the Schläfli symbol, gives a combinatorial description of the polyhedron. The Schläfli symbols of the five Platonic solids are given in the table below.

Properties of Platonic solids

Polyhedron		Vertices	Edges	Faces	Schläfli symbol	Vertex configuration
Regular tetrahedron		4	6	4	{3, 3}	3.3.3
cube		8	12	6	{4, 3}	4.4.4
Regular octahedron		6	12	8	{3, 4}	3.3.3.3
Regular dodecahedron		20	30	12	{5, 3}	5.5.5
Regular icosahedron		12	30	20	{3, 5}	3.3.3.3.3

All other combinatorial information about these solids, such as total number of vertices (V), edges (E), and faces (F), can be determined from p and q. Since any edge joins two vertices and has two adjacent faces we must have:

p F = 2 E = q V . {\displaystyle pF=2E=qV.\,}

The other relationship between these values is given by Euler's formula:

V − E + F = 2. {\displaystyle V-E+F=2.\,}

This can be proved in many ways. Together these three relationships completely determine V, E, and F:

V = 4 p 4 − ( p − 2 ) ( q − 2 ) , E = 2 p q 4 − ( p − 2 ) ( q − 2 ) , F = 4 q 4 − ( p − 2 ) ( q − 2 ) . {\displaystyle V={\frac {4p}{4-(p-2)(q-2)}},\quad E={\frac {2pq}{4-(p-2)(q-2)}},\quad F={\frac {4q}{4-(p-2)(q-2)}}.}

Swapping p and q interchanges F and V while leaving E unchanged. For a geometric interpretation of this property, see § Dual polyhedra.

The elements of a polyhedron can be expressed in a configuration matrix. The rows and columns correspond to vertices, edges, and faces. The diagonal numbers say how many of each element occur in the whole polyhedron. The nondiagonal numbers say how many of the column's element occur in or at the row's element. Dual pairs of polyhedra have their configuration matrices rotated 180 degrees from each other.^[8]

{p,q}	Platonic configurations
Group order: g = 8pq/(4 − (p − 2)(q − 2))	g = 24	g = 48		g = 120
v e f v g/2q q q e 2 g/4 2 f p p g/2p	{3,3} 4 3 3 2 6 2 3 3 4	{3,4} 6 4 4 2 12 2 3 3 8	{4,3} 8 3 3 2 12 2 4 4 6	{3,5} 12 5 5 2 30 2 3 3 20	{5,3} 20 3 3 2 30 2 5 5 12

The classical result is that only five convex regular polyhedra exist. Two common arguments below demonstrate no more than five Platonic solids can exist, but positively demonstrating the existence of any given solid is a separate question—one that requires an explicit construction.

Polygon nets around a vertex

{3,3} Defect 180°	{3,4} Defect 120°	{3,5} Defect 60°	{3,6} Defect 0°
{4,3} Defect 90°	{4,4} Defect 0°	{5,3} Defect 36°	{6,3} Defect 0°
A vertex needs at least 3 faces, and an angle defect. A 0° angle defect will fill the Euclidean plane with a regular tiling. By Descartes' theorem, the number of vertices is 720°/defect.

The following geometric argument is very similar to the one given by Euclid in the Elements:

A purely topological proof can be made using only combinatorial information about the solids. The key is Euler's observation that V − E + F = 2, and the fact that pF = 2E = qV, where p stands for the number of edges of each face and q for the number of edges meeting at each vertex. Combining these equations one obtains the equation

2 E q − E + 2 E p = 2. {\displaystyle {\frac {2E}{q}}-E+{\frac {2E}{p}}=2.}

Simple algebraic manipulation then gives

1 q + 1 p = 1 2 + 1 E . {\displaystyle {1 \over q}+{1 \over p}={1 \over 2}+{1 \over E}.}

Since E is strictly positive we must have

1 q + 1 p > 1 2 . {\displaystyle {\frac {1}{q}}+{\frac {1}{p}}>{\frac {1}{2}}.}

Using the fact that p and q must both be at least 3, one can easily see that there are only five possibilities for {p, q}:

There are a number of angles associated with each Platonic solid. The dihedral angle is the interior angle between any two face planes. The dihedral angle, θ, of the solid {p,q} is given by the formula

sin ⁡ ( θ / 2 ) = cos ⁡ ( π / q ) sin ⁡ ( π / p ) . {\displaystyle \sin(\theta /2)={\frac {\cos(\pi /q)}{\sin(\pi /p)}}.}

This is sometimes more conveniently expressed in terms of the tangent by

tan ⁡ ( θ / 2 ) = cos ⁡ ( π / q ) sin ⁡ ( π / h ) . {\displaystyle \tan(\theta /2)={\frac {\cos(\pi /q)}{\sin(\pi /h)}}.}

The quantity h (called the Coxeter number) is 4, 6, 6, 10, and 10 for the tetrahedron, cube, octahedron, dodecahedron, and icosahedron respectively.

The angular deficiency at the vertex of a polyhedron is the difference between the sum of the face-angles at that vertex and 2π. The defect, δ, at any vertex of the Platonic solids {p,q} is

δ = 2 π − q π ( 1 − 2 p ) . {\displaystyle \delta =2\pi -q\pi \left(1-{2 \over p}\right).}

By a theorem of Descartes, this is equal to 4π divided by the number of vertices (i.e. the total defect at all vertices is 4π).

The three-dimensional analog of a plane angle is a solid angle. The solid angle, Ω, at the vertex of a Platonic solid is given in terms of the dihedral angle by

Ω = q θ − ( q − 2 ) π . {\displaystyle \Omega =q\theta -(q-2)\pi .\,}

This follows from the spherical excess formula for a spherical polygon and the fact that the vertex figure of the polyhedron {p,q} is a regular q-gon.

The solid angle of a face subtended from the center of a platonic solid is equal to the solid angle of a full sphere (4π steradians) divided by the number of faces. This is equal to the angular deficiency of its dual.

The various angles associated with the Platonic solids are tabulated below. The numerical values of the solid angles are given in steradians. The constant φ = ⁠1 + √5/2⁠ is the golden ratio.

Polyhedron	Dihedral angle (θ)	tan ⁠θ/2⁠	Defect (δ)	Vertex solid angle (Ω)	Face solid angle
tetrahedron	70.53°	1 2 {\displaystyle 1 \over {\sqrt {2}}}	π {\displaystyle \pi }	arccos ⁡ ( 23 27 ) ≈ 0.551286 {\displaystyle \arccos \left({\frac {23}{27}}\right)\quad \approx 0.551286}	π {\displaystyle \pi }
cube	90°	1 {\displaystyle 1}	π 2 {\displaystyle \pi \over 2}	π 2 ≈ 1.57080 {\displaystyle {\frac {\pi }{2}}\quad \approx 1.57080}	2 π 3 {\displaystyle 2\pi \over 3}
octahedron	109.47°	2 {\displaystyle {\sqrt {2}}}	2 π 3 {\displaystyle {2\pi } \over 3}	4 arcsin ⁡ ( 1 3 ) ≈ 1.35935 {\displaystyle 4\arcsin \left({1 \over 3}\right)\quad \approx 1.35935}	π 2 {\displaystyle \pi \over 2}
dodecahedron	116.57°	φ {\displaystyle \varphi }	π 5 {\displaystyle \pi \over 5}	π − arctan ⁡ ( 2 11 ) ≈ 2.96174 {\displaystyle \pi -\arctan \left({\frac {2}{11}}\right)\quad \approx 2.96174}	π 3 {\displaystyle \pi \over 3}
icosahedron	138.19°	φ 2 {\displaystyle \varphi ^{2}}	π 3 {\displaystyle \pi \over 3}	2 π − 5 arcsin ⁡ ( 2 3 ) ≈ 2.63455 {\displaystyle 2\pi -5\arcsin \left({2 \over 3}\right)\quad \approx 2.63455}	π 5 {\displaystyle \pi \over 5}

Another virtue of regularity is that the Platonic solids all possess three concentric spheres:

• the circumscribed sphere that passes through all the vertices,
• the midsphere that is tangent to each edge at the midpoint of the edge, and
• the inscribed sphere that is tangent to each face at the center of the face.

The radii of these spheres are called the circumradius, the midradius, and the inradius. These are the distances from the center of the polyhedron to the vertices, edge midpoints, and face centers respectively. The circumradius R and the inradius r of the solid {p, q} with edge length a are given by

R = a 2 tan ⁡ ( π q ) tan ⁡ ( θ 2 ) r = a 2 cot ⁡ ( π p ) tan ⁡ ( θ 2 ) {\displaystyle {\begin{aligned}R&={\frac {a}{2}}\tan \left({\frac {\pi }{q}}\right)\tan \left({\frac {\theta }{2}}\right)\\[3pt]r&={\frac {a}{2}}\cot \left({\frac {\pi }{p}}\right)\tan \left({\frac {\theta }{2}}\right)\end{aligned}}}

where θ is the dihedral angle. The midradius ρ is given by

ρ = a 2 cos ⁡ ( π p ) csc ( π h ) {\displaystyle \rho ={\frac {a}{2}}\cos \left({\frac {\pi }{p}}\right)\,{\csc }{\biggl (}{\frac {\pi }{h}}{\biggr )}}

where h is the quantity used above in the definition of the dihedral angle (h = 4, 6, 6, 10, or 10). The ratio of the circumradius to the inradius is symmetric in p and q:

R r = tan ⁡ ( π p ) tan ⁡ ( π q ) = csc 2 ( θ 2 ) − cos 2 ( α 2 ) sin ⁡ ( α 2 ) . {\displaystyle {\frac {R}{r}}=\tan \left({\frac {\pi }{p}}\right)\tan \left({\frac {\pi }{q}}\right)={\frac {\sqrt {{\csc ^{2}}{\Bigl (}{\frac {\theta }{2}}{\Bigr )}-{\cos ^{2}}{\Bigl (}{\frac {\alpha }{2}}{\Bigr )}}}{\sin {\Bigl (}{\frac {\alpha }{2}}{\Bigr )}}}.}

The surface area, A, of a Platonic solid {p, q} is easily computed as area of a regular p-gon times the number of faces F. This is:

A = ( a 2 ) 2 F p cot ⁡ ( π p ) . {\displaystyle A={\biggl (}{\frac {a}{2}}{\biggr )}^{2}Fp\cot \left({\frac {\pi }{p}}\right).}

The volume is computed as F times the volume of the pyramid whose base is a regular p-gon and whose height is the inradius r. That is,

V = 1 3 r A . {\displaystyle V={\frac {1}{3}}rA.}

The following table lists the various radii of the Platonic solids together with their surface area and volume. The overall size is fixed by taking the edge length, a, to be equal to 2.

Polyhedron, a = 2	Radius			Surface area, A	Volume
	In-, r	Mid-, ρ	Circum-, R		V	Unit edges
tetrahedron	1 6 {\displaystyle 1 \over {\sqrt {6}}}	1 2 {\displaystyle 1 \over {\sqrt {2}}}	3 2 {\displaystyle {\sqrt {3 \over 2}}}	4 3 {\displaystyle 4{\sqrt {3}}}	8 3 ≈ 0.942809 {\displaystyle {\frac {\sqrt {8}}{3}}\approx 0.942809}	≈ 0.117851 {\displaystyle \approx 0.117851}
cube	1 {\displaystyle 1\,}	2 {\displaystyle {\sqrt {2}}}	3 {\displaystyle {\sqrt {3}}}	24 {\displaystyle 24\,}	8 {\displaystyle 8\,}	1 {\displaystyle 1\,}
octahedron	2 3 {\displaystyle {\sqrt {2 \over 3}}}	1 {\displaystyle 1\,}	2 {\displaystyle {\sqrt {2}}}	8 3 {\displaystyle 8{\sqrt {3}}}	128 3 ≈ 3.771236 {\displaystyle {\frac {\sqrt {128}}{3}}\approx 3.771236}	≈ 0.471404 {\displaystyle \approx 0.471404}
dodecahedron	φ 2 ξ {\displaystyle {\frac {\varphi ^{2}}{\xi }}}	φ 2 {\displaystyle \varphi ^{2}}	3 φ {\displaystyle {\sqrt {3}}\,\varphi }	12 25 + 10 5 {\displaystyle 12{\sqrt {25+10{\sqrt {5}}}}}	20 φ 3 ξ 2 ≈ 61.304952 {\displaystyle {\frac {20\varphi ^{3}}{\xi ^{2}}}\approx 61.304952}	≈ 7.663119 {\displaystyle \approx 7.663119}
icosahedron	φ 2 3 {\displaystyle {\frac {\varphi ^{2}}{\sqrt {3}}}}	φ {\displaystyle \varphi }	ξ φ {\displaystyle \xi \varphi }	20 3 {\displaystyle 20{\sqrt {3}}}	20 φ 2 3 ≈ 17.453560 {\displaystyle {\frac {20\varphi ^{2}}{3}}\approx 17.453560}	≈ 2.181695 {\displaystyle \approx 2.181695}

The constants φ and ξ in the above are given by

φ = 2 cos ⁡ π 5 = 1 + 5 2 , ξ = 2 sin ⁡ π 5 = 5 − 5 2 = 3 − φ . {\displaystyle \varphi =2\cos {\pi \over 5}={\frac {1+{\sqrt {5}}}{2}},\qquad \xi =2\sin {\pi \over 5}={\sqrt {\frac {5-{\sqrt {5}}}{2}}}={\sqrt {3-\varphi }}.}

Among the Platonic solids, either the dodecahedron or the icosahedron may be seen as the best approximation to the sphere. The icosahedron has the largest number of faces and the largest dihedral angle, it hugs its inscribed sphere the most tightly, and its surface area to volume ratio is closest to that of a sphere of the same size (i.e. either the same surface area or the same volume). The dodecahedron, on the other hand, has the smallest angular defect, the largest vertex solid angle, and it fills out its circumscribed sphere the most.

For an arbitrary point in the space of a Platonic solid with circumradius R, whose distances to the centroid of the Platonic solid and its n vertices are L and d_i respectively, and

S [ n ] ( 2 m ) = 1 n ∑ i = 1 n d i 2 m {\displaystyle S_{[n]}^{(2m)}={\frac {1}{n}}\sum _{i=1}^{n}d_{i}^{2m}} ,

we have^[9]

S [ 4 ] ( 2 ) = S [ 6 ] ( 2 ) = S [ 8 ] ( 2 ) = S [ 12 ] ( 2 ) = S [ 20 ] ( 2 ) = R 2 + L 2 , S [ 4 ] ( 4 ) = S [ 6 ] ( 4 ) = S [ 8 ] ( 4 ) = S [ 12 ] ( 4 ) = S [ 20 ] ( 4 ) = ( R 2 + L 2 ) 2 + 4 3 R 2 L 2 , S [ 6 ] ( 6 ) = S [ 8 ] ( 6 ) = S [ 12 ] ( 6 ) = S [ 20 ] ( 6 ) = ( R 2 + L 2 ) 3 + 4 R 2 L 2 ( R 2 + L 2 ) , S [ 12 ] ( 8 ) = S [ 20 ] ( 8 ) = ( R 2 + L 2 ) 4 + 8 R 2 L 2 ( R 2 + L 2 ) 2 + 16 5 R 4 L 4 , S [ 12 ] ( 10 ) = S [ 20 ] ( 10 ) = ( R 2 + L 2 ) 5 + 40 3 R 2 L 2 ( R 2 + L 2 ) 3 + 16 R 4 L 4 ( R 2 + L 2 ) . {\displaystyle {\begin{aligned}S_{[4]}^{(2)}=S_{[6]}^{(2)}=S_{[8]}^{(2)}=S_{[12]}^{(2)}=S_{[20]}^{(2)}&=R^{2}+L^{2},\\[4px]S_{[4]}^{(4)}=S_{[6]}^{(4)}=S_{[8]}^{(4)}=S_{[12]}^{(4)}=S_{[20]}^{(4)}&=\left(R^{2}+L^{2}\right)^{2}+{\frac {4}{3}}R^{2}L^{2},\\[4px]S_{[6]}^{(6)}=S_{[8]}^{(6)}=S_{[12]}^{(6)}=S_{[20]}^{(6)}&=\left(R^{2}+L^{2}\right)^{3}+4R^{2}L^{2}\left(R^{2}+L^{2}\right),\\[4px]S_{[12]}^{(8)}=S_{[20]}^{(8)}&=\left(R^{2}+L^{2}\right)^{4}+8R^{2}L^{2}\left(R^{2}+L^{2}\right)^{2}+{\frac {16}{5}}R^{4}L^{4},\\[4px]S_{[12]}^{(10)}=S_{[20]}^{(10)}&=\left(R^{2}+L^{2}\right)^{5}+{\frac {40}{3}}R^{2}L^{2}\left(R^{2}+L^{2}\right)^{3}+16R^{4}L^{4}\left(R^{2}+L^{2}\right).\end{aligned}}} For all five Platonic solids, we have^[9]

S [ n ] ( 4 ) + 16 9 R 4 = ( S [ n ] ( 2 ) + 2 3 R 2 ) 2 . {\displaystyle S_{[n]}^{(4)}+{\frac {16}{9}}R^{4}=\left(S_{[n]}^{(2)}+{\frac {2}{3}}R^{2}\right)^{2}.}

If d_i are the distances from the n vertices of the Platonic solid to any point on its circumscribed sphere, then^[9]

4 ( ∑ i = 1 n d i 2 ) 2 = 3 n ∑ i = 1 n d i 4 . {\displaystyle 4\left(\sum _{i=1}^{n}d_{i}^{2}\right)^{2}=3n\sum _{i=1}^{n}d_{i}^{4}.}

A polyhedron P is said to have the Rupert property if a polyhedron of the same or larger size and the same shape as P can pass through a hole in P.^[10] All five Platonic solids have this property.^[10][11][12]

Every polyhedron has a dual (or "polar") polyhedron with faces and vertices interchanged. The dual of every Platonic solid is another Platonic solid, so that we can arrange the five solids into dual pairs.

• The tetrahedron is self-dual (i.e. its dual is another tetrahedron).
• The cube and the octahedron form a dual pair.
• The dodecahedron and the icosahedron form a dual pair.

If a polyhedron has Schläfli symbol {p, q}, then its dual has the symbol {q, p}. Indeed, every combinatorial property of one Platonic solid can be interpreted as another combinatorial property of the dual.

One can construct the dual polyhedron by taking the vertices of the dual to be the centers of the faces of the original figure. Connecting the centers of adjacent faces in the original forms the edges of the dual and thereby interchanges the number of faces and vertices while maintaining the number of edges.

More generally, one can dualize a Platonic solid with respect to a sphere of radius d concentric with the solid. The radii (R, ρ, r) of a solid and those of its dual (R*, ρ*, r*) are related by

d 2 = R ∗ r = r ∗ R = ρ ∗ ρ . {\displaystyle d^{2}=R^{\ast }r=r^{\ast }R=\rho ^{\ast }\rho .}

Dualizing with respect to the midsphere (d = ρ) is often convenient because the midsphere has the same relationship to both polyhedra. Taking d² = Rr yields a dual solid with the same circumradius and inradius (i.e. R* = R and r* = r).

In mathematics, the concept of symmetry is studied with the notion of a mathematical group. Every polyhedron has an associated symmetry group, which is the set of all transformations (Euclidean isometries) which leave the polyhedron invariant. The order of the symmetry group is the number of symmetries of the polyhedron. One often distinguishes between the full symmetry group, which includes reflections, and the proper symmetry group, which includes only rotations.

The symmetry groups of the Platonic solids are a special class of three-dimensional point groups known as polyhedral groups. The high degree of symmetry of the Platonic solids can be interpreted in a number of ways. Most importantly, the vertices of each solid are all equivalent under the action of the symmetry group, as are the edges and faces. One says the action of the symmetry group is transitive on the vertices, edges, and faces. In fact, this is another way of defining regularity of a polyhedron: a polyhedron is regular if and only if it is vertex-uniform, edge-uniform, and face-uniform.

There are only three symmetry groups associated with the Platonic solids rather than five, since the symmetry group of any polyhedron coincides with that of its dual. This is easily seen by examining the construction of the dual polyhedron. Any symmetry of the original must be a symmetry of the dual and vice versa. The three polyhedral groups are:

• the tetrahedral group T,
• the octahedral group O (which is also the symmetry group of the cube), and
• the icosahedral group I (which is also the symmetry group of the dodecahedron).

The orders of the proper (rotation) groups are 12, 24, and 60 respectively – precisely twice the number of edges in the respective polyhedra. The orders of the full symmetry groups are twice as much again (24, 48, and 120). See (Coxeter 1973) for a derivation of these facts. All Platonic solids except the tetrahedron are centrally symmetric, meaning they are preserved under reflection through the origin.

The following table lists the various symmetry properties of the Platonic solids. The symmetry groups listed are the full groups with the rotation subgroups given in parentheses (likewise for the number of symmetries). Wythoff's kaleidoscope construction is a method for constructing polyhedra directly from their symmetry groups. They are listed for reference Wythoff's symbol for each of the Platonic solids.

Polyhedron	Schläfli symbol	Wythoff symbol	Dual polyhedron	Symmetry group (reflection, rotation)
				Polyhedral	Schön.	Cox.	Orb.	Order
tetrahedron	{3, 3}	3 | 2 3	tetrahedron	Tetrahedral	Td T	[3,3] [3,3]+	*332 332	24 12
cube	{4, 3}	3 | 2 4	octahedron	Octahedral	Oh O	[4,3] [4,3]+	*432 432	48 24
octahedron	{3, 4}	4 | 2 3	cube
dodecahedron	{5, 3}	3 | 2 5	icosahedron	Icosahedral	Ih I	[5,3] [5,3]+	*532 532	120 60
icosahedron	{3, 5}	5 | 2 3	dodecahedron

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The tetrahedron, cube, and octahedron all occur naturally in crystal structures. These by no means exhaust the numbers of possible forms of crystals. However, neither the regular icosahedron nor the regular dodecahedron are amongst them. One of the forms, called the pyritohedron (named for the group of minerals of which it is typical) has twelve pentagonal faces, arranged in the same pattern as the faces of the regular dodecahedron. The faces of the pyritohedron are, however, not regular, so the pyritohedron is also not regular. Allotropes of boron and many boron compounds, such as boron carbide, include discrete B₁₂ icosahedra within their crystal structures. Carborane acids also have molecular structures approximating regular icosahedra.

In the early 20th century, Ernst Haeckel described a number of species of Radiolaria, some of whose skeletons are shaped like various regular polyhedra. Examples include Circoporus octahedrus, Circogonia icosahedra, Lithocubus geometricus and Circorrhegma dodecahedra. The shapes of these creatures should be obvious from their names.^[13]

Many viruses, such as the herpes^[14] virus, have the shape of a regular icosahedron. Viral structures are built of repeated identical protein subunits and the icosahedron is the easiest shape to assemble using these subunits. A regular polyhedron is used because it can be built from a single basic unit protein used over and over again; this saves space in the viral genome.

In meteorology and climatology, global numerical models of atmospheric flow are of increasing interest which employ geodesic grids that are based on an icosahedron (refined by triangulation) instead of the more commonly used longitude/latitude grid. This has the advantage of evenly distributed spatial resolution without singularities (i.e. the poles) at the expense of somewhat greater numerical difficulty.

Geometry of space frames is often based on platonic solids. In the MERO system, Platonic solids are used for naming convention of various space frame configurations. For example, ⁠1/2⁠O+T refers to a configuration made of one half of octahedron and a tetrahedron.

Several Platonic hydrocarbons have been synthesised, including cubane and dodecahedrane.

• 
  Tetrahedrane
• 
  Cubane
• 
  Dodecahedrane

For the intermediate material phase called liquid crystals, the existence of such symmetries was first proposed in 1981 by H. Kleinert and K. Maki.^[15][16] In aluminum the icosahedral structure was discovered three years after this by Dan Shechtman, which earned him the Nobel Prize in Chemistry in 2011.

Platonic solids are often used to make dice, because dice of these shapes can be made fair. 6-sided dice are very common, but the other numbers are commonly used in role-playing games. Such dice are commonly referred to as dn where n is the number of faces (d8, d20, etc.); see dice notation for more details.

These shapes frequently show up in other games or puzzles. Puzzles similar to a Rubik's Cube come in all five shapes – see magic polyhedra.

Architects liked the idea of Plato's timeless forms that can be seen by the soul in the objects of the material world, but turned these shapes into more suitable for construction sphere, cylinder, cone, and square pyramid.^[17] In particular, one of the leaders of neoclassicism, Étienne-Louis Boullée, was preoccupied with the architects' version of "Platonic solids".^[18]

• 
  Icosahedron as a part of Spinoza monument in Amsterdam
• 
  Solar cube at Discovery Cube Orange County
• 
  Octahedron under construction in Austria
• 
  Tetrahedron in Bottrop
• 
  Dodecahedron in Budapest

There exist four regular polyhedra that are not convex, called Kepler–Poinsot polyhedra. These all have icosahedral symmetry and may be obtained as stellations of the dodecahedron and the icosahedron.

cuboctahedron

icosidodecahedron

The next most regular convex polyhedra after the Platonic solids are the cuboctahedron, which is a rectification of the cube and the octahedron, and the icosidodecahedron, which is a rectification of the dodecahedron and the icosahedron (the rectification of the self-dual tetrahedron is a regular octahedron). These are both quasi-regular, meaning that they are vertex- and edge-uniform and have regular faces, but the faces are not all congruent (coming in two different classes). They form two of the thirteen Archimedean solids, which are the convex uniform polyhedra with polyhedral symmetry. Their duals, the rhombic dodecahedron and rhombic triacontahedron, are edge- and face-transitive, but their faces are not regular and their vertices come in two types each; they are two of the thirteen Catalan solids.

The uniform polyhedra form a much broader class of polyhedra. These figures are vertex-uniform and have one or more types of regular or star polygons for faces. These include all the polyhedra mentioned above together with an infinite set of prisms, an infinite set of antiprisms, and 53 other non-convex forms.

The Johnson solids are convex polyhedra which have regular faces but are not uniform. Among them are five of the eight convex deltahedra, which have identical, regular faces (all equilateral triangles) but are not uniform. (The other three convex deltahedra are the Platonic tetrahedron, octahedron, and icosahedron.)

Regular spherical tilings

Platonic
{3,3}	{4,3}	{3,4}	{5,3}	{3,5}
Regular dihedral
{2,2}	{3,2}	{4,2}	{5,2}	{6,2}...
Regular hosohedral
{2,2}	{2,3}	{2,4}	{2,5}	{2,6}...

The three regular tessellations of the plane are closely related to the Platonic solids. Indeed, one can view the Platonic solids as regular tessellations of the sphere. This is done by projecting each solid onto a concentric sphere. The faces project onto regular spherical polygons which exactly cover the sphere. Spherical tilings provide two infinite additional sets of regular tilings, the hosohedra, {2,n} with 2 vertices at the poles, and lune faces, and the dual dihedra, {n,2} with 2 hemispherical faces and regularly spaced vertices on the equator. Such tesselations would be degenerate in true 3D space as polyhedra.

Every regular tessellation of the sphere is characterized by a pair of integers {p, q} with ⁠1/p⁠ + ⁠1/q⁠ > ⁠1/2⁠. Likewise, a regular tessellation of the plane is characterized by the condition ⁠1/p⁠ + ⁠1/q⁠ = ⁠1/2⁠. There are three possibilities:

The three regular tilings of the Euclidean plane

{4, 4}	{3, 6}	{6, 3}

In a similar manner, one can consider regular tessellations of the hyperbolic plane. These are characterized by the condition ⁠1/p⁠ + ⁠1/q⁠ < ⁠1/2⁠. There is an infinite family of such tessellations.

Example regular tilings of the hyperbolic plane

{5, 4}	{4, 5}	{7, 3}	{3, 7}

Number of dimensions	Number of convex regular polytopes
0	1
1	1
2	∞
3	5
4	6
> 4	3

In more than three dimensions, polyhedra generalize to polytopes, with higher-dimensional convex regular polytopes being the equivalents of the three-dimensional Platonic solids.

In the mid-19th century the Swiss mathematician Ludwig Schläfli discovered the four-dimensional analogues of the Platonic solids, called convex regular 4-polytopes. There are exactly six of these figures; five are analogous to the Platonic solids : 5-cell as {3,3,3}, 16-cell as {3,3,4}, 600-cell as {3,3,5}, tesseract as {4,3,3}, and 120-cell as {5,3,3}, and a sixth one, the self-dual 24-cell, {3,4,3}.

In all dimensions higher than four, there are only three convex regular polytopes: the simplex as {3,3,...,3}, the hypercube as {4,3,...,3}, and the cross-polytope as {3,3,...,4}.^[19] In three dimensions, these coincide with the tetrahedron as {3,3}, the cube as {4,3}, and the octahedron as {3,4}.

• Atiyah, Michael; Sutcliffe, Paul (2003). "Polyhedra in Physics, Chemistry and Geometry". Milan J. Math. 71: 33–58. arXiv:math-ph/0303071. Bibcode:2003math.ph...3071A. doi:10.1007/s00032-003-0014-1. S2CID 119725110.
• Boyer, Carl; Merzbach, Uta (1989). A History of Mathematics (2nd ed.). Wiley. ISBN 0-471-54397-7.
• Coxeter, H. S. M. (1973). Regular Polytopes (3rd ed.). New York: Dover Publications. ISBN 0-486-61480-8.
• Cromwell, Peter R. (1997). Polyhedra. Cambridge University Press. ISBN 9780521554329.
• Euclid (1980) [1st pub. 1956]. Heath, Thomas L. (ed.). The Thirteen Books of Euclid's Elements, Books 10–13 (2nd unabr. ed.). New York: Dover Publications. ISBN 0-486-60090-4.
• Gardner, Martin (1987). The 2nd Scientific American Book of Mathematical Puzzles & Diversions, University of Chicago Press, Chapter 1: The Five Platonic Solids, ISBN 0226282538
• Gelernter, Mark (1995). Sources of Architectural Form: A Critical History of Western Design Theory. Manchester University Press. ISBN 978-0-7190-4129-7. Retrieved 2024-02-12.
• Kepler. Johannes Strena seu de nive sexangula (On the Six-Cornered Snowflake), 1611 paper by Kepler which discussed the reason for the six-angled shape of the snow crystals and the forms and symmetries in nature. Talks about platonic solids.
• Kleinert, Hagen & Maki, K. (1981). "Lattice Textures in Cholesteric Liquid Crystals" (PDF). Fortschritte der Physik. 29 (5): 219–259. Bibcode:1981ForPh..29..219K. doi:10.1002/prop.19810290503.
• Lloyd, David Robert (2012). "How old are the Platonic Solids?". BSHM Bulletin: Journal of the British Society for the History of Mathematics. 27 (3): 131–140. doi:10.1080/17498430.2012.670845. S2CID 119544202.
• * Olenick, R. P.; Apostol, T. M.; Goodstein, D. L. (1986). The Mechanical Universe: Introduction to Mechanics and Heat. Cambridge University Press. ISBN 0-521-30429-6.
• Pugh, Anthony (1976). Polyhedra: A visual approach. California: University of California Press Berkeley. ISBN 0-520-03056-7.
• Weyl, Hermann (1980) [1st pub. 1952]. Symmetry. Princeton, NJ: Princeton University Press. ISBN 0-691-02374-3.
• Wildberg, Christian (1988). John Philoponus' Criticism of Aristotle's Theory of Aether. Walter de Gruyter. pp. 11–12. ISBN 9783110104462.

This section's use of external links may not follow Wikipedia's policies or guidelines. Please improve this article by removing excessive or inappropriate external links, and converting useful links where appropriate into footnote references. (December 2019) (Learn how and when to remove this message)

• Platonic solids at Encyclopaedia of Mathematics
• Weisstein, Eric W. "Platonic solid". MathWorld.
• Weisstein, Eric W. "Isohedron". MathWorld.
• Book XIII of Euclid's Elements.
• Interactive 3D Polyhedra in Java
• Platonic Solids in Visual Polyhedra
• Solid Body Viewer is an interactive 3D polyhedron viewer which allows you to save the model in svg, stl or obj format.
• Interactive Folding/Unfolding Platonic Solids Archived 2007-02-09 at the Wayback Machine in Java
• Paper models of the Platonic solids created using nets generated by Stella software
• Platonic Solids Free paper models (nets)
• Grime, James; Steckles, Katie. "Platonic Solids". Numberphile. Brady Haran. Archived from the original on 2018-10-23. Retrieved 2013-04-13.
• Teaching Math with Art student-created models
• Teaching Math with Art teacher instructions for making models
• Frames of Platonic Solids images of algebraic surfaces
• Platonic Solids with some formula derivations
• How to make four platonic solids from a cube