View source for 120-cell

{{Short description|Four-dimensional analog of the dodecahedron}}
{{Infobox polychoron
|  Name=120-cell
|  Image_File=Schlegel wireframe 120-cell.png
|  Image_Caption=[[Schlegel diagram]]<br>(vertices and edges)
|  Type=[[Convex regular 4-polytope]]
|  Last=[[Snub 24-cell|31]]
|  Index=32
|  Next=[[Rectified 120-cell|33]]
|  Schläfli={5,3,3}|
  CD={{CDD|node_1|5|node|3|node|3|node}}|
  Cell_List=120 [[Dodecahedron|{5,3}]] [[Image:Dodecahedron.png|20px]]|
  Face_List=720 [[pentagon|{5}]] [[File:Regular pentagon.svg|20px]]|
  Edge_Count=1200|
  Vertex_Count= 600|
  Petrie_Polygon=[[triacontagon|30-gon]]|
  Coxeter_Group=H<sub>4</sub>, [3,3,5]|
  Vertex_Figure=[[File:120-cell verf.svg|80px]]<br>[[tetrahedron]]|
  Dual=[[600-cell]]|
  Property_List=[[convex set|convex]], [[isogonal figure|isogonal]], [[isotoxal figure|isotoxal]], [[isohedral figure|isohedral]]
}}
[[File:120-cell net.png|thumb|right|[[Net (polyhedron)|Net]]]]
In [[geometry]], the '''120-cell''' is the [[convex regular 4-polytope]] (four-dimensional analogue of a [[Platonic solid]]) with [[Schläfli symbol]] {5,3,3}. It is also called a '''C<sub>120</sub>''',  '''dodecaplex''' (short for "dodecahedral complex"), '''hyperdodecahedron''', '''polydodecahedron''', '''hecatonicosachoron''', '''dodecacontachoron'''<ref>[[Norman Johnson (mathematician)|N.W. Johnson]]: ''Geometries and Transformations'', (2018) {{ISBN|978-1-107-10340-5}} Chapter 11: ''Finite Symmetry Groups'', 11.5 ''Spherical Coxeter groups'', p.249</ref> and '''hecatonicosahedroid'''.<ref>Matila Ghyka, ''The Geometry of Art and Life'' (1977), p.68</ref>

The boundary of the 120-cell is composed of 120 dodecahedral [[cell (mathematics)|cells]] with 4 meeting at each vertex. Together they form 720 [[Pentagon|pentagonal]] faces, 1200 edges, and 600 vertices. It is the 4-[[Four-dimensional space#Dimensional analogy|dimensional analogue]] of the [[regular dodecahedron]], since just as a dodecahedron has 12 pentagonal facets, with 3 around each vertex, the ''dodecaplex'' has 120 dodecahedral facets, with 3 around each edge.{{Efn|In the 120-cell, 3 dodecahedra and 3 pentagons meet at every edge. 4 dodecahedra, 6 pentagons, and 4 edges meet at every vertex. The dihedral angle (between dodecahedral hyperplanes) is 144°.{{Sfn|Coxeter|1973|loc=Table I(ii); "120-cell"|pp=292-293}}|name=dihedral}} Its dual polytope is the [[600-cell]].

== Geometry ==
The 120-cell incorporates the geometries of every convex regular polytope in the first four dimensions (except the polygons {7} and above).{{Efn|name=elements}} As the sixth and largest regular convex 4-polytope,{{Efn|The convex regular 4-polytopes can be ordered by size as a measure of 4-dimensional content (hypervolume) for the same radius. Each greater polytope in the sequence is ''rounder'' than its predecessor, enclosing more 4-content within the same radius. The 4-simplex (5-cell) is the limit smallest case, and the 120-cell is the largest. Complexity (as measured by comparing [[#As a configuration|configuration matrices]] or simply the number of vertices) follows the same ordering. This provides an alternative numerical naming scheme for regular polytopes in which the 120-cell is the 600-point 4-polytope: sixth and last in the ascending sequence that begins with the 5-point 4-polytope.|name=polytopes ordered by size and complexity}} it contains inscribed instances of its four predecessors (recursively). It also contains 120 inscribed instances of the first in the sequence, the [[5-cell]],{{Efn|name=inscribed 5-cells}} which is not found in any of the others.{{Sfn|Dechant|2021|p=18|loc=''Remark 5.7''|ps=, explains why not.{{Efn|name=rotated 4-simplexes are completely disjoint}}}} The 120-cell is a four-dimensional [[Swiss Army knife]]: it contains one of everything.

It is daunting but instructive to study the 120-cell, because it contains examples of ''every'' relationship among ''all'' the convex regular polytopes found in the first four dimensions. Conversely, it can only be understood by first understanding each of its predecessors, and the sequence of increasingly complex symmetries they exhibit.{{Sfn|Dechant|2021|loc=Abstract|ps=; "[E]very 3D root system allows the construction of a corresponding 4D root system via an ‘induction theorem’. In this paper, we look at the icosahedral case of H3 → H4 in detail
and perform the calculations explicitly. Clifford algebra is used to perform group theoretic calculations based on the versor theorem and the Cartan-Dieudonné theorem ... shed[ding] light on geometric aspects of the H4 root system (the 600-cell) as well as other related polytopes and their symmetries ... including the construction of the Coxeter plane, which is used for visualising the complementary pairs of invariant polytopes.... This approach therefore constitutes a more systematic and general way of performing calculations concerning groups, in particular reflection groups and root systems, in a Clifford algebraic framework."}} That is why [[John Stillwell|Stillwell]] titled his paper on the 4-polytopes and the history of mathematics<ref>''Mathematics and Its History'', John Stillwell, 1989, 3rd edition 2010, {{isbn|0-387-95336-1}}</ref> of more than 3 dimensions ''The Story of the 120-cell''.{{Sfn|Stillwell|2001}}

{{Regular convex 4-polytopes}}

===Cartesian coordinates===
Natural Cartesian coordinates for a 4-polytope centered at the origin of 4-space occur in different frames of reference, depending on the long radius (center-to-vertex) chosen.

==== √8 radius coordinates ====
The 120-cell with long radius {{Radic|8}} = 2{{Radic|2}} ≈ 2.828 has edge length  4−2φ = 3−{{radic|5}} ≈ 0.764.  

In this frame of reference, its 600 vertex coordinates are the {[[permutations]]} and {{bracket|[[even permutation]]s}} of the following:{{Sfn|Coxeter|1973|loc=§8.7 Cartesian coordinates|pp=156-157}} 
{| class=wikitable
|-
!24
| ({0, 0, ±2, ±2})
| [[24-cell#Squares|24-cell]]
| rowspan=7 | 600-point 120-cell
|-
!64
| ({±φ, ±φ, ±φ, ±φ<sup>−2</sup>})
|
|-
!64
| ({±1, ±1, ±1, ±{{radic|5}}<nowiki />})
|
|-
!64
| ({±φ<sup>−1</sup>, ±φ<sup>−1</sup>, ±φ<sup>−1</sup>, ±φ<sup>2</sup>})
|
|-
!96
| ([0, ±φ<sup>−1</sup>, ±φ, ±{{radic|5}}])
| [[Snub 24-cell#Coordinates|Snub 24-cell]]
|-
!96
| ([0, ±φ<sup>−2</sup>, ±1, ±φ<sup>2</sup>])
| [[Snub 24-cell#Coordinates|Snub 24-cell]]
|-
!192
| ([±φ<sup>−1</sup>, ±1, ±φ, ±2])
|
|}

where φ (also called 𝝉){{Efn|{{Harv|Coxeter|1973}} uses the greek letter 𝝓 (phi) to represent one of the three ''characteristic angles'' 𝟀, 𝝓, 𝟁 of a regular polytope. Because 𝝓 is commonly used to represent the [[golden ratio]] constant ≈ 1.618, for which Coxeter uses 𝝉 (tau), we reverse Coxeter's conventions, and use 𝝉 to represent the characteristic angle.|name=reversed greek symbols}} is the [[golden ratio]], {{sfrac|1 + {{radic|5}}|2}} ≈ 1.618.

==== Unit radius coordinates ====
The unit-radius 120-cell has edge length {{Sfrac|1|φ<sup>2</sup>{{Radic|2}}}} ≈ 0.270. 

In this frame of reference the 120-cell lies vertex up in standard orientation, and its coordinates{{Sfn|Mamone|Pileio|Levitt|2010|p=1442|loc=Table 3}} are the {[[permutations]]} and {{bracket|[[even permutation]]s}} in the left column below:
{| class="wikitable" style=width:720px
|-
!rowspan=3|120
!8
|style="white-space: nowrap;"|({±1, 0, 0, 0})
|[[16-cell#Coordinates|16-cell]]
| rowspan="2" |[[24-cell#Hexagons|24-cell]]
| rowspan="3" |[[600-cell#Coordinates|600-cell]]
| rowspan="10" style="white-space: nowrap;"|120-cell
|-
!16
|style="white-space: nowrap;"|({±1, ±1, ±1, ±1}) / 2
|[[Tesseract#Radial equilateral symmetry|Tesseract]]
|-
!96
|style="white-space: nowrap;"|([0, ±φ<sup>−1</sup>, ±1, ±φ]) / 2
|colspan=2|[[Snub 24-cell#Coordinates|Snub 24-cell]]
|-
!rowspan=7|480
!colspan=2|[[#Tetrahedrally diminished 120-cell|Diminished 120-cell]]
!5-point [[5-cell#Coordinates|5-cell]]
![[24-cell#Squares|24-cell]]
![[600-cell#Coordinates|600-cell]]
|-
!32
|style="white-space: nowrap;"|([±φ, ±φ, ±φ, ±φ<sup>−2</sup>]) / {{radic|8}}
|rowspan=6 style="white-space: nowrap;"|(1, 0, 0, 0)<br>
(−1,{{spaces|2}}{{radic|5}},{{spaces|2}}{{radic|5}},{{spaces|2}}{{radic|5}}) / 4<br>
(−1,−{{radic|5}},−{{radic|5}},{{spaces|2}}{{radic|5}}) / 4<br>
(−1,−{{radic|5}},{{spaces|2}}{{radic|5}},−{{radic|5}}) / 4<br>
(−1,{{spaces|2}}{{radic|5}},−{{radic|5}},−{{radic|5}}) / 4
|rowspan=6 style="white-space: nowrap;"|({±{{radic|1/2}}, ±{{radic|1/2}}, 0, 0})
|rowspan=6 style="white-space: nowrap;"|({±1, 0, 0, 0})<br>
({±1, ±1, ±1, ±1}) / 2<br>
([0, ±φ<sup>−1</sup>, ±1, ±φ]) / 2
|-
!32
|style="white-space: nowrap;"|([±1, ±1, ±1, ±{{radic|5}}]) / {{radic|8}}
|-
!32
|style="white-space: nowrap;"|([±φ<sup>−1</sup>, ±φ<sup>−1</sup>, ±φ<sup>−1</sup>, ±φ<sup>2</sup>]) / {{radic|8}}
|-
!96
|style="white-space: nowrap;"|([0, ±φ<sup>−1</sup>, ±φ, ±{{radic|5}}]) / {{radic|8}}
|-
!96
|style="white-space: nowrap;"|([0, ±φ<sup>−2</sup>, ±1, ±φ<sup>2</sup>]) / {{radic|8}}
|-
!192
|style="white-space: nowrap;"|([±φ<sup>−1</sup>, ±1, ±φ, ±2]) / {{radic|8}}
|-
|colspan=7|The unit-radius coordinates of uniform convex 4-polytopes are related by [[quaternion]] multiplication. Since the regular 4-polytopes are compounds of each other, their sets of Cartesian 4-coordinates (quaternions) are set products of each other. The unit-radius coordinates of the 600 vertices of the 120-cell (in the left column above) are all the possible [[Quaternion#Multiplication of basis elements|quaternion products]]{{Sfn|Mamone|Pileio|Levitt|2010|p=1433|loc=§4.1|ps=; A Cartesian 4-coordinate point (w,x,y,z) is a vector in 4D space from (0,0,0,0). Four-dimensional real space is a vector space: any two vectors can be added or multiplied by a scalar to give another vector. Quaternions extend the vectorial structure of 4D real space by allowing the multiplication of two 4D vectors  <small><math>\left(w,x,y,z\right)_1</math></small> and <small><math>\left(w,x,y,z\right)_2</math></small> according to<br>
<small><math display=block>\begin{pmatrix}
w_2\\
x_2\\
y_2\\
z_2
\end{pmatrix}
*
\begin{pmatrix}
w_1\\
x_1\\
y_1\\
z_1
\end{pmatrix}
=
\begin{pmatrix}
{w_2 w_1 - x_2 x_1 - y_2 y_1 - z_2 z_1}\\
{w_2 x_1 + x_2 w_1 + y_2 z_1 - z_2 y_1}\\
{w_2 y_1 - x_2 z_1 + y_2 w_1 + z_2 x_1}\\
{w_2 z_1 + x_2 y_1 - y_2 x_1 + z_2 w_1}
\end{pmatrix}
</math></small>}} of the 5 vertices of the 5-cell, the 24 vertices of the 24-cell, and the 120 vertices of the 600-cell (in the other three columns above).{{Efn|To obtain all 600 coordinates by quaternion cross-multiplication of these three 4-polytopes' coordinates with less redundancy, it is sufficient to include just one vertex of the 24-cell: ({{radic|1/2}}, {{radic|1/2}}, 0, 0).{{Sfn|Mamone|Pileio|Levitt|2010|loc=Table 3|p=1442}}}}
|}

The table gives the coordinates of at least one instance of each 4-polytope, but the 120-cell contains multiples-of-five inscribed instances of each of its precursor 4-polytopes, occupying different subsets of its vertices. The (600-point) 120-cell is the convex hull of 5 disjoint (120-point) 600-cells. Each (120-point) 600-cell is the convex hull of 5 disjoint (24-point) 24-cells, so the 120-cell is the convex hull of 25 disjoint 24-cells. Each 24-cell is the convex hull of 3 disjoint (8-point) 16-cells, so the 120-cell is the convex hull of 75 disjoint 16-cells. Uniquely, the (600-point) 120-cell is the convex hull of 120 disjoint (5-point) 5-cells.{{Efn|The 120-cell can be constructed as a compound of '''{{red|5}}''' disjoint 600-cells,{{Efn|name=2 ways to get 5 disjoint 600-cells}} or '''{{red|25}}''' disjoint 24-cells, or '''{{red|75}}''' disjoint 16-cells, or '''{{red|120}}''' disjoint 5-cells. Except in the case of the 120 5-cells,{{Efn|Multiple instances of each of the regular convex 4-polytopes can be inscribed in any of their larger successor 4-polytopes, except for the smallest, the regular 5-cell, which occurs inscribed only in the largest, the 120-cell.{{Efn|name=simplex-orthoplex-cube relation}} To understand the way in which the 4-polytopes nest within each other, it is necessary to carefully distinguish ''disjoint'' multiple instances from merely ''distinct'' multiple instances of inscribed 4-polytopes. For example, the 600-point 120-cell is the convex hull of a compound of 75 8-point 16-cells that are completely disjoint: they share no vertices, and 75 * 8 {{=}} 600. But it is also possible to pick out 675 distinct 16-cells within the 120-cell, most pairs of which share some vertices, because two concentric equal-radius 16-cells may be rotated with respect to each other such that they share 2 vertices (an axis), or even 4 vertices (a great square plane), while their remaining vertices are not coincident.{{Efn|name=rays and bases}} In 4-space, any two congruent regular 4-polytopes may be concentric but rotated with respect to each other such that they share only a common subset of their vertices. Only in the case of the 4-simplex (the 5-point regular 5-cell) that common subset of vertices must always be empty, unless it is all 5 vertices. It is impossible to rotate two concentric 4-simplexes with respect to each other such that some, but not all, of their vertices are coincident: they may only be completely coincident, or completely disjoint. Only the 4-simplex has this property; the 16-cell, and by extension any larger regular 4-polytope, may lie rotated with respect to itself such that the pair shares some, but not all, of their vertices. Intuitively we may see how this follows from the fact that only the 4-simplex does not possess any opposing vertices (any 2-vertex central axes) which might be invariant after a rotation. The 120-cell contains 120 completely disjoint regular 5-cells, which are its only distinct inscribed regular 5-cells, but every other nesting of regular 4-polytopes features some number of disjoint inscribed 4-polytopes and a larger number of distinct inscribed 4-polytopes.|name=rotated 4-simplexes are completely disjoint}} these are not counts of ''all'' the distinct regular 4-polytopes which can be found inscribed in the 120-cell, only the counts of ''completely disjoint'' inscribed 4-polytopes which when compounded form the convex hull of the 120-cell. The 120-cell contains '''{{green|10}}''' distinct 600-cells, '''{{green|225}}''' distinct 24-cells, and '''{{green|675}}''' distinct 16-cells.{{Efn|name=rays and bases}}|name=inscribed counts}}

===Chords===
[[File:Great polygons of the 120-cell.png|thumb|300px|Great circle polygons of the 120-cell, which lie in the invariant central planes of its isoclinic{{Efn|Two angles are required to specify the separation between two planes in 4-space.{{Sfn|Kim|Rote|2016|p=7|loc=§6 Angles between two Planes in 4-Space|ps=; "In four (and higher) dimensions, we need two angles to fix the relative position between two planes. (More generally, ''k'' angles are defined between ''k''-dimensional subspaces.)".}} If the two angles are identical, the two planes are called isoclinic (also [[Clifford parallel]]) and they intersect in a single point. In [[Rotations in 4-dimensional Euclidean space#Double rotations|double rotations]], points rotate within invariant central planes of rotation by some angle, and the entire invariant central plane of rotation also tilts sideways (in an orthogonal invariant central plane of rotation) by some angle. Therefore each vertex traverses a ''helical'' smooth curve called an ''isocline''{{Efn|An '''isocline''' is a closed, curved, helical great circle through all four dimensions. Unlike an ordinary great circle it does not lie in a single central plane, but like any great circle, when viewed within the curved 3-dimensional space of the 4-polytope's boundary surface it is a ''straight line'', a [[geodesic]]. Both ordinary great circles and isocline great circles are helical in the sense that parallel bundles of great circles are [[Link (knot theory)|linked]] and spiral around each other, but neither are actually twisted (they have no inherent torsion). Their curvature is not their own, but a property of the 3-sphere's natural curvature, within which curved space they are finite (closed) straight line segments.{{Efn|name=isocline circumference}} To avoid confusion, we always refer to an ''isocline'' as such, and reserve the term ''[[great circle]]'' for an ordinary great circle in the plane.{{Efn|name=isocline circumference}}|name=isocline}} between two points in different central planes, while traversing an ordinary great circle in each of two orthogonal central planes (as the planes tilt relative to their original planes). If the two orthogonal angles are identical, the distance traveled along each great circle is the same, and the double rotation is called isoclinic (also a [[SO(4)#Isoclinic rotations|Clifford displacement]]). A rotation which takes isoclinic central planes to each other is an isoclinic rotation.{{Efn|name=isoclinic rotation}}|name=isoclinic}} rotations. The 120-cell edges of length {{Color|red|𝜁}} ≈ 0.270 occur only in the {{Color|red|red}} irregular great hexagon, which also has edges of length {{Color|red|{{radic|2.5}}}}. The 120-cell's 1200 edges do not form great circle polygons by themselves, but by alternating with {{radic|2.5}} edges of inscribed regular 5-cells{{Efn|name=inscribed 5-cells}} they form 400 irregular great hexagons.{{Efn|name=irregular great hexagon}} The 120-cell also contains a compound of several of these great circle polygons in the same central plane, illustrated separately.{{Efn|name=irregular great dodecagon}} An implication of the compounding is that the edges and characteristic rotations{{Efn|name=characteristic rotation}} of the regular 5-cell, the 8-cell hypercube, the 24-cell, and the 120-cell all lie in the same rotation planes, the hexagonal central planes of the 24-cell.{{Efn|name=edge rotation planes}}]]
{{see also|600-cell#Golden chords}}

The 600-point 120-cell has all 8 of the 120-point 600-cell's distinct chord lengths, plus two additional important chords: its own shorter edges, and the edges of its 120 inscribed regular 5-cells.{{Efn|[[File:Regular_star_figure_6(5,2).svg|thumb|200px|In [[Triacontagon#Triacontagram|triacontagram {30/12}=6{5/2}]],<br> six of the 120 disjoint regular 5-cells of edge-length {{radic|2.5}} which are inscribed in the 120-cell appear as six pentagrams, the [[5-cell#Boerdijk–Coxeter helix|Clifford polygon of the 5-cell]]. The 30 vertices comprise a Petrie polygon of the 120-cell,{{Efn|name=two coaxial Petrie 30-gons}} with 30 zig-zag edges (not shown), and 3 inscribed great decagons (edges not shown) which lie Clifford parallel to the projection plane.{{Efn|Inscribed in the 3 Clifford parallel great decagons of each helical Petrie polygon of the 120-cell{{Efn|name=inscribed 5-cells}} are 6 great pentagons{{Efn|In [[600-cell#Decagons and 5𝝅 polygrams|600-cell § Decagons and pentadecagrams]], see the illustration of [[Triacontagon#Triacontagram|triacontagram {30/6}=6{5}]].}} in which the 6 pentagrams (regular 5-cells) appear to be inscribed, but the pentagrams are skew (not parallel to the projection plane); each 5-cell actually has vertices in 5 different decagon-pentagon central planes in 5 completely disjoint 600-cells.|name=great pentagon}}]]Inscribed in the unit-radius 120-cell are 120 disjoint regular 5-cells,{{Sfn|Coxeter|1973|loc=Table VI (iv): 𝐈𝐈 = {5,3,3}|p=304}} of edge-length {{radic|2.5}}. No regular 4-polytopes except the 5-cell and the 120-cell contain {{radic|2.5}} chords (the #8 chord).{{Efn|name=rotated 4-simplexes are completely disjoint}} The 120-cell contains 10 distinct inscribed 600-cells which can be taken as 5 disjoint 600-cells two different ways. Each {{radic|2.5}} chord connects two vertices in disjoint 600-cells, and hence in disjoint 24-cells, 8-cells, and 16-cells.{{Efn|name=simplex-orthoplex-cube relation}} Both the 5-cell edges and the 120-cell edges connect vertices in disjoint 600-cells. Corresponding polytopes of the same kind in disjoint 600-cells are Clifford parallel and {{radic|2.5}} apart. Each 5-cell contains one vertex from each of 5 disjoint 600-cells.{{Efn|The 120 regular 5-cells are completely disjoint. Each 5-cell contains two distinct Petrie pentagons of its #8 edges, [[5-cell#Geodesics and rotations|pentagonal circuits]] each binding 5 disjoint 600-cells together in a distinct isoclinic rotation characteristic of the 5-cell. But the vertices of two ''disjoint 5-cells'' are not linked by 5-cell edges, so each distinct circuit of #8 chords is confined to a single 5-cell, and there are no other circuits of 5-cell edges (#8 chords) in the 120-cell.|name=distinct circuits of the 5-cell}}.|name=inscribed 5-cells}} These two additional chords give the 120-cell its characteristic [[SO(4)#Isoclinic rotations|isoclinic rotation]],{{Efn|[[File:Regular_star_figure_2(15,4).svg|thumb|200px|In [[Triacontagon#Triacontagram|triacontagram {30/8}=2{15/4}]],<br>2 disjoint [[pentadecagram]] isoclines are visible: a black and a white isocline (shown here as orange and faint yellow) of the 120-cell's characteristic isoclinic rotation.{{Efn|Each black or white pentadecagram isocline acts as both a right isocline in a distinct right isoclinic rotation and as a left isocline in a distinct left isoclinic rotation, but isoclines do not have inherent chirality.{{Efn|name=isocline}} No isocline is both a right and left isocline of the ''same'' discrete left-right rotation (the same fibration).}} The pentadecagram edges are #4 chords{{Efn|name=#4 isocline chord}} joining vertices which are 8 vertices apart on the 30-vertex circumference of this projection, the zig-zag Petrie polygon.{{Efn|name=pentadecagram isoclines}}]]The characteristic isoclinic rotation{{Efn|name=characteristic rotation}} of the 120-cell takes place in the invariant planes of its 1200 edges{{Efn|name=non-planar geodesic circle}} and [[5-cell#Geodesics and rotations|its inscribed regular 5-cells' opposing 1200 edges]].{{Efn|The invariant central plane of the 120-cell's characteristic isoclinic rotation{{Efn|name=120-cell characteristic rotation}} contains an irregular great hexagon {6} with alternating edges of two different lengths: 3 120-cell edges of length 𝜁 {{=}} {{radic|0.𝜀}} (#1 chords), and 3 inscribed regular 5-cell edges of length {{radic|2.5}} (#8 chords). These are, respectively, the shortest and longest edges of any regular 4-polytope. {{Efn|Each {{radic|2.5}} chord is spanned by 8 zig-zag edges of a Petrie 30-gon,{{Efn|name=120-cell Petrie {30}-gon}} none of which lie in the great circle of the irregular great hexagon. Alternately the {{radic|2.5}} chord is spanned by 9 zig-zag edges, one of which (over its midpoint) does lie in the same great circle.{{Efn|name=irregular great hexagon}}|name=spanned by 8 or 9 edges}} Each irregular great hexagon lies completely orthogonal to another irregular great hexagon.{{Efn|name=perpendicular and parallel}} The 120-cell contains 400 distinct irregular great hexagons (200 completely orthogonal pairs), which can be partitioned into 100 disjoint irregular great hexagons (a discrete fibration of the 120-cell) in four different ways. Each fibration has its distinct left (and right) isoclinic rotation in 50 pairs of completely orthogonal invariant central planes. Two irregular great hexagons occupy the same central plane, in alternate positions, just as two great pentagons occupy a great decagon plane. The two irregular great hexagons form an irregular great dodecagon, a compound [[#Chords|great circle polygon of the 120-cell]] which is illustrated separately.{{Efn|name=irregular great dodecagon}}|name=irregular great hexagon}} There are four distinct characteristic right (and left) isoclinic rotations, each left-right pair corresponding to a discrete [[Hopf fibration]].{{Sfn|Mamone|Pileio|Levitt|2010|loc=§4.5 Regular Convex 4-Polytopes, Table 2, Symmetry operations|pp=1438-1439|ps=; in symmetry group 𝛢<sub>4</sub> the operation [15]𝑹<sub>q3,q3</sub> is the 15 distinct rotational displacements which comprise the class of [[5-cell#Geodesics and rotations|pentagram isoclinic rotations of an individual 5-cell]]; in symmetry group 𝛨<sub>4</sub> the operation [1200]𝑹<sub>q3,q13</sub> is the 1200 distinct rotational displacements which comprise the class of pentadecagram isoclinic rotations of the 120-cell, the 120-cell's characteristic rotation.}} In each rotation all 600 vertices circulate on helical isoclines of 15 vertices, following a geodesic circle{{Efn|name=isocline}} with 15 #4 chords that form a {15/4} pentadecagram.{{Efn|The characteristic isocline{{Efn|name=isocline}} of the 120-cell is a skew pentadecagram of 15 #4 chords. Successive #4 chords of each pentadecagram lie in different △ central planes which are inclined isoclinically to each other at 12°, which is 1/30 of a great circle (but not the arc of a 120-cell edge, the #1 chord).{{Efn|name=12° rotation angle}} This means that the two planes are separated by two equal 12° angles,{{Efn|name=isoclinic}} and they are occupied by adjacent [[Clifford parallel]] great polygons (irregular great hexagons) whose corresponding vertices are joined by oblique #4 chords. Successive vertices of each pentadecagram are vertices in completely disjoint 5-cells. Each pentadecagram is a #4 chord-path{{Efn|name=non-planar geodesic circle}} visiting 15 vertices belonging to three different 5-cells. The two pentadecagrams shown in the {30/8}{{=}}2{15/4} projection{{Efn|name=120-cell characteristic rotation}} visit the six 5-cells that appear as six disjoint pentagrams in the {30/12}{{=}}6{5/2} projection.{{Efn|name=inscribed 5-cells}}|name=pentadecagram isoclines}}|name=120-cell characteristic rotation}} in addition to all the rotations of the other regular 4-polytopes which it inherits.{{Sfn|Mamone|Pileio|Levitt|2010|loc=§4.5 Regular Convex 4-Polytopes, Table 2, Symmetry group 𝛨<sub>4</sub>|pp=1438-1439|ps=; the 120-cell has 7200 distinct rotational displacements (and 7200 reflections), which can be grouped as 25 distinct ''isoclinic'' rotations.{{Efn|name=distinct rotations}}}} They also give the 120-cell a characteristic great circle polygon: an ''irregular'' great hexagon in which three 120-cell edges alternate with three 5-cell edges.{{Efn|name=irregular great hexagon}}

The 120-cell's edges do not form regular great circle polygons in a single central plane the way the edges of the 600-cell, 24-cell, and 16-cell do. Like the edges of the [[5-cell#Geodesics and rotations|5-cell]] and the [[8-cell|8-cell tesseract]], they form zig-zag [[Petrie polygon]]s instead.{{Efn|The 5-cell, 8-cell and 120-cell all have tetrahedral vertex figures. In a 4-polytope with a tetrahedral vertex figure, a path along edges does not lie on an ordinary great circle in a single central plane: each successive edge lies in a different central plane than the previous edge. In the 120-cell the 30-edge circumferential path along edges follows a zig-zag skew Petrie polygon, which is not a great circle. However, there exists a 15-chord circumferential path that is a true geodesic great circle through those 15 vertices: but it is not an ordinary "flat" great circle of circumference 2𝝅𝑟, it is a helical ''isocline''{{Efn|name=isocline}} that bends in a circle in two completely orthogonal central planes at once, circling through four dimensions rather than confined to a two dimensional plane.{{Efn|name=pentadecagram isoclines}} The skew chord set of an isocline is called its ''Clifford polygon''.{{Efn|name=Clifford polygon}}|name=non-planar geodesic circle}} The [[Petrie polygon#The Petrie polygon of regular polychora (4-polytopes)|120-cell's Petrie polygon]] is a [[triacontagon]] {30} zig-zag [[Skew polygon#Regular skew polygons in four dimensions|skew polygon]].{{Efn|[[File:Regular polygon 30.svg|thumb|200px|The Petrie polygon of the 120-cell is a [[skew polygon|skew]] regular [[triacontagon]] {30}.{{Efn|name=15 distinct chord lengths}} The 30 #1 chord edges do not all lie on the same {30} great circle polygon, but they lie in groups of 6 (equally spaced around the circumference) in 5 Clifford parallel {12} great circle polygons.{{Efn|name=irregular great dodecagon}}]]The 120-cell contains 80 distinct [[30-gon]] Petrie polygons of its 1200 edges, and can be partitioned into 20 disjoint 30-gon Petrie polygons.{{Efn|name=Petrie polygons of the 120-cell}} The Petrie 30-gon twists around its 0-gon great circle axis 9 times in the course of one circular orbit, and can be seen as a compound [[Triacontagon#Triacontagram|triacontagram {30/9}{{=}}3{10/3}]] of 600-cell edges (#3 chords) linking pairs of vertices that are 9 vertices apart on the Petrie polygon.{{Efn|name=two coaxial Petrie 30-gons}} The {30/9}-gram (with its #3 chord edges) is an alternate sequence of the same 30 vertices as the Petrie 30-gon (with its #1 chord edges).|name=120-cell Petrie {30}-gon}}

Since the 120-cell has a circumference of 30 edges, it has 15 distinct chord lengths, ranging from its edge length to its diameter.{{Efn|The 30-edge circumference of the 120-cell follows a skew Petrie polygon, not a great circle polygon. The Petrie polygon of any 4-polytope is a zig-zag helix spiraling through the curved 3-space of the 4-polytope's surface.{{Efn|The Petrie polygon of a 3-polytope (polyhedron) with triangular faces (e.g. an icosahedron) can be seen as a linear strip of edge-bonded faces bent into a ring. Within that circular strip of edge-bonded triangles (10 in the case of the icosahedron) the [[Petrie polygon]] can be picked out as a [[skew polygon]] of edges zig-zagging (not circling) through the 2-space of the polyhedron's surface: alternately bending left and right, and slaloming around a great circle axis that passes through the triangles but does not intersect any vertices. The Petrie polygon of a 4-polytope (polychoron) with tetrahedral cells (e.g. a 600-cell) can be seen as a linear helix of face-bonded cells bent into a ring: a [[600-cell#Boerdijk–Coxeter helix rings|Boerdijk–Coxeter helix ring]]. Within that circular helix of face-bonded tetrahedra (30 in the case of the 600-cell) the skew Petrie polygon can be picked out as a helix of edges zig-zagging (not circling) through the 3-space of the polychoron's surface: alternately bending left and right, and spiraling around a great circle axis that passes through the tetrahedra but does not intersect any vertices.}} The 15 numbered [[#Chords|chords]] of the 120-cell occur as the distance between two vertices in that 30-vertex helical ring.{{Efn|name=additional 120-cell chords}} Those 15 distinct [[Pythagorean distance]]s through 4-space range from the 120-cell edge-length which links any two nearest vertices in the ring (the #1 chord), to the 120-cell axis-length (diameter) which links any two antipodal (most distant) vertices in the ring (the #15 chord).|name=15 distinct chord lengths}} Every regular convex 4-polytope is inscribed in the 120-cell, and the 15 chords enumerated in the rows of the following table are all the distinct chords that make up the regular 4-polytopes and their great circle polygons.{{Efn|The 120-cell itself contains more chords than the 15 chords numbered #1 - #15, but the additional chords occur only in the interior of 120-cell, not as edges of any of the six regular convex 4-polytopes or their characteristic great circle rings. The 15 ''[[#Chords|major chords]]'' are so numbered because the #''n'' chord connects two vertices which are ''n'' edge lengths apart on a Petrie polygon. There are [[#Geodesic rectangles|30 distinct 4-space chordal distances]] between vertices of the 120-cell (15 pairs of 180° complements), including #15 the 180° diameter (and its complement the 0° chord). In this article, we name the 15 unnumbered ''minor chords'' by their arc-angles, e.g. 41.4~° which, with length {{radic|0.5}}, falls between the #3 and #4 chords.|name=additional 120-cell chords}}

The first thing to notice about this table is that it has eight columns, not six; in addition to the six regular convex 4-polytopes, two irregular 4-polytopes occur naturally in the sequence of nested 4-polytopes: the 96-point [[snub 24-cell]] and the 480-point [[#Tetrahedrally diminished 120-cell|diminished 120-cell]].{{Efn|name=polytopes ordered by size and complexity}}

The second thing to notice is that each numbered row is marked with a triangle △, square ☐, or pentagon ✩. The 15 chords lie in [[600-cell#Geodesics|central planes]] of three kinds: great square ☐ planes [[16-cell#Coordinates|characteristic of the 16-cell]], great hexagon and great triangle △ planes [[24-cell#Hexagons|characteristic of the 24-cell]], or great decagon and great pentagon ✩ planes [[600-cell#Hopf spherical coordinates|characteristic of the 600-cell]].{{Efn|The edges and 4𝝅 characteristic rotations of the [[16-cell#Coordinates|16-cell]] lie in the great square ☐ central planes. Rotations of this type are an expression of the [[Hyperoctahedral group|symmetry group <math>B_4</math>]]. The edges and 5𝝅 characteristic rotations of the [[600-cell#Hopf spherical coordinates|600-cell]] lie in the great pentagon ✩ (great decagon) central planes. Rotations of this type are an expression of the [[H4 polytope|symmetry group <math>H_4</math>]]. The edges and characteristic rotations{{Efn|name=isocline circumference}} of the other regular 4-polytopes, the regular [[5-cell#Geodesics and rotations|5-cell]], the [[Tesseract|8-cell hypercube]], the [[24-cell#Hexagons|24-cell]], and the 120-cell,{{Efn|name=120-cell characteristic rotation}} all lie in the great triangle △ (great hexagon) central planes.{{Efn|name=irregular great dodecagon}} Collectively these rotations are expressions of all four symmetry groups [[Tetrahedral symmetry|<math>A_4</math>]], [[Hyperoctahedral group|<math>B_4</math>]], [[F4 (mathematics)|<math>F_4</math>]] and [[H4 polytope|<math>H_4</math>]].|name=edge rotation planes}}

{| class=wikitable style="white-space:nowrap;text-align:center"
!colspan=14|Chords of the 120-cell and its inscribed 4-polytopes{{Sfn|Coxeter|1973|pp=300-301|loc=Table V:(v) Simplified sections of {5,3,3} (edge 2φ<sup>−2</sup>√2 [radius 4]) beginning with a vertex|ps=; Coxeter's table lists 16 non-point sections labelled 1<sub>0</sub> − 16<sub>0</sub>, polyhedra whose successively increasing "radii" on the 3-sphere (in column 2''la'') are the following chords in our notation:{{Efn|name=additional 120-cell chords}} #1, #2, #3, 41.4~°, #4, 49.1~°, 56.0~°, #5, 66.1~°, 69.8~°, #6, 75.5~°, 81.1~°, 84.5~°, #7, 95.5~°, ..., #15. The remaining distinct chords occur as the longer "radii" of the second set of 16 opposing polyhedral sections (in column ''a'' for (30−''i'')<sub>0</sub>) which lists #15, #14, #13, #12, 138.6~°, #11, 130.1~°, 124~°, #10, 113.9~°, 110.2~°, #9, #8, 98.9~°, 95.5~°, #7, 84.5~°, ..., or at least they occur among the 180° complements of all those Coxeter-listed chords. The complete ordered set of 30 distinct chords is 0°, #1, #2, #3, 41.4~°, #4, 49.1~°, 56~°, #5, 66.1~°, 69.8~°, #6, 75.5~°, 81.1~°, 84.5~°, #7, 95.5~°, #8, #9, 110.2°, 113.9°, #10, 124°, 130.1°, #11, 138.6°, #12, #13, #14, #15. The chords also occur among the edge-lengths of the polyhedral sections (in column 2''lb'', which lists only: #2, .., #3, .., 69.8~°, .., .., #3, .., .., #5, #8, .., .., .., #7, ... because the multiple edge-lengths of irregular polyhedral sections are not given).}}
|-
!colspan=5|Inscribed{{Efn|"At a point of contact, [elements of a regular polytope and elements of its dual in which it is inscribed in some manner] lie in completely orthogonal subspaces of the tangent hyperplane to the sphere [of reciprocation], so their only common point is the point of contact itself.... In fact, the [various] radii <sub>0</sub>𝑹, <sub>1</sub>𝑹, <sub>2</sub>𝑹, ... determine the polytopes ... whose vertices are the centers of elements 𝐈𝐈<sub>0</sub>, 𝐈𝐈<sub>1</sub>, 𝐈𝐈<sub>2</sub>, ... of the original polytope."{{Sfn|Coxeter|1973|p=147|loc=§8.1 The simple truncations of the general regular polytope}}|name=Coxeter on orthogonal dual pairs}}
![[5-cell]]
![[16-cell]]
![[8-cell]]
![[24-cell]]
![[Snub 24-cell|Snub]]
![[600-cell]]
![[#Tetrahedrally diminished 120-cell|Dimin]]
! style="border-right: none;"|120-cell
! style="border-left: none;"|
|-
!colspan=5|Vertices
| style="background: seashell;"|5
| style="background: paleturquoise;"|8
| style="background: paleturquoise;"|16
| style="background: paleturquoise;"|24
| style="background: yellow;"|96
| style="background: yellow;"|120
| style="background: seashell;"|480
| style="background: seashell; border-right: none;"|600{{Efn|name=rays and bases}}
|rowspan=6 style="background: seashell; border: none;"|
|-
!colspan=5|Edges
| style="background: seashell;"|10{{Efn|name=irregular great hexagon}}
| style="background: paleturquoise;"|24
| style="background: paleturquoise;"|32
| style="background: paleturquoise;"|96
| style="background: yellow;"|432
| style="background: yellow;"|720
| style="background: seashell;"|1200
| style="background: seashell;"|1200{{Efn|name=irregular great hexagon}}
|-
!colspan=5|Edge chord
| style="background: seashell;"|#8{{Efn|name=inscribed 5-cells}}
| style="background: paleturquoise;"|#7
| style="background: paleturquoise;"|#5
| style="background: paleturquoise;"|#5
| style="background: yellow;"|#3
| style="background: yellow;"|#3{{Efn|[[File:Regular_star_figure_3(10,3).svg|180px|thumb|In [[Triacontagon#Triacontagram|triacontagram {30/9}{{=}}3{10/3}]] we see the 120-cell Petrie polygon (on the circumference of the 30-gon, with 120-cell edges not shown) as a compound of three Clifford parallel 600-cell great decagons (seen as three disjoint {10/3} decagrams) that spiral around each other. The 600-cell edges (#3 chords) connect vertices which are 3 600-cell edges apart (on a great circle), and 9 120-cell edges apart (on a Petrie polygon). The three disjoint {10/3} great decagons of 600-cell edges delineate a single [[600-cell#Boerdijk–Coxeter helix rings|Boerdijk–Coxeter helix 30-tetrahedron ring]] of an inscribed 600-cell.]] The 120-cell and 600-cell both have 30-gon Petrie polygons.{{Efn|The [[Skew polygon#Regular skew polygons in four dimensions|regular skew 30-gon]] is the [[Petrie polygon]] of the [[600-cell]] and its dual the 120-cell. The Petrie polygons of the 120-cell occur in the 600-cell as duals of the 30-cell [[600-cell#Boerdijk–Coxeter helix rings|Boerdijk–Coxeter helix rings]] (the Petrie polygons of the 600-cell):{{Efn|[[File:Regular_star_polygon_30-11.svg|180px|thumb|The Petrie polygon of the inscribed 600-cells can be seen in this projection to the plane of a triacontagram {30/11}, a 30-gram of #11 chords. The 600-cell Petrie  is a helical ring which winds around its own axis 11 times. This projection along the axis of the ring cylinder shows the 30 vertices 12° apart around the cylinder's circular cross section, with #11 chords connecting every 11th vertex on the circle. The 600-cell edges (#3 chords) which are the Petrie polygon edges are not shown in this illustration, but they could be drawn around the circumference, connecting every 3rd vertex.]]The [[600-cell#Boerdijk–Coxeter helix rings|600-cell Petrie polygon is a helical ring]] which twists around its 0-gon great circle axis 11 times in the course of one circular orbit. Projected to the plane completely orthogonal to the 0-gon plane, the 600-cell Petrie polygon can be seen to be a [[Triacontagon#Triacontagram|triacontagram {30/11}]] of 30 #11 chords linking pairs of vertices that are 11 vertices apart on the circumference of the projection.{{Sfn|Sadoc|2001|pp=577-578|loc=§2.5 The 30/11 symmetry: an example of other kind of symmetries}} The {30/11}-gram (with its #11 chord edges) is an alternate sequence of the same 30 vertices as the Petrie 30-gon (with its #3 chord edges).|name={30/11}-gram}} connecting their 30 tetrahedral cell centers together produces the Petrie polygons of the dual 120-cell, as noticed by Rolfdieter Frank (circa 2001). Thus he discovered that the vertex set of the 120-cell partitions into 20 non-intersecting Petrie polygons. This set of 20 disjoint Clifford parallel skew polygons is a discrete [[Hopf fibration]] of the 120-cell (just as their 20 dual 30-cell rings are a [[600-cell#Decagons|discrete fibration of the 600-cell]]).{{Efn|name=two coaxial Petrie 30-gons}}|name=Petrie polygons of the 120-cell}} They are two distinct skew 30-gon helices, composed of 30 120-cell edges (#1 chords) and 30 600-cell edges (#3 chords) respectively, but they occur in completely orthogonal pairs that spiral around the same 0-gon great circle axis. The 120-cell's Petrie helix winds closer to the axis than the [[600-cell#Boerdijk–Coxeter helix rings|600-cell's Petrie helix]] does, because its 30 edges are shorter than the 600-cell's 30 edges (and they zig-zag at less acute angles). A dual pair{{Efn|name=Petrie polygons of the 120-cell}} of these Petrie helices of different radii sharing an axis do not have any vertices in common; they are completely disjoint.{{Efn|name=Coxeter on orthogonal dual pairs}} The 120-cell Petrie helix (versus the 600-cell Petrie helix) twists around the 0-gon axis 9 times (versus 11 times) in the course of one circular orbit, forming a skew [[Triacontagon#Triacontagram|{30/9}{{=}}3{10/3} polygram]] (versus a skew [[Triacontagon#Triacontagram|{30/11} polygram]]).{{Efn|name={30/11}-gram}}|name=two coaxial Petrie 30-gons}}
| style="background: seashell;"|#1
| style="background: seashell;"|#1{{Efn|name=120-cell Petrie {30}-gon}}
|-
!colspan=5|[[600-cell#Rotations on polygram isoclines|Isocline chord]]{{Efn|name=isoclinic rotation}}
| style="background: seashell;"|[[5-cell#Geodesics and rotations|#8]]
| style="background: paleturquoise;"|[[16-cell#Helical construction|#15]]
| style="background: paleturquoise;"|#10
| style="background: paleturquoise;"|[[24-cell#Helical hexagrams and their isoclines|#10]]
| style="background: yellow;"|#5
| style="background: yellow;"|[[600-cell#Decagons and 5𝝅 polygrams|#5]]
| style="background: seashell;"|#4
| style="background: seashell;"|#4{{Efn|name=#4 isocline chord}}
|-
!colspan=5|Clifford polygon{{Efn|The chord-path of an isocline{{Efn|name=isocline}} may be called the 4-polytope's ''Clifford polygon'', as it is the skew polygram shape of the rotational circles traversed by the 4-polytope's vertices in its characteristic [[Clifford displacement]].{{Efn|name=isoclinic}}|name=Clifford polygon}}
| style="background: seashell;"|[[5-cell#Boerdijk–Coxeter helix|{5/2}]]
| style="background: paleturquoise;"|[[16-cell#Helical construction|{8/3}]]
| style="background: paleturquoise;"|{{^|[[hexagram|{6/2}]]}}
| style="background: paleturquoise;"|[[24-cell#Helical hexagrams and their isoclines|{6/2}]]
| style="background: yellow;"|{{^|[[pentadecagram|{15/2}]]}}
| style="background: yellow;"|[[600-cell#Decagons and 5𝝅 polygrams|{15/2}]]
| style="background: seashell;"|{{^|[[pentadecagram|{15/4}]]}}
| style="background: seashell;"|[[pentadecagram|{15/4}]]{{Efn|name=120-cell characteristic rotation}}
|-
!colspan=2|Chord
!Arc
!colspan=2|Edge
| style="background: seashell;"|
| style="background: paleturquoise;"|
| style="background: paleturquoise;"|
| style="background: paleturquoise;"|
| style="background: yellow;"|
| style="background: yellow;"|
| style="background: seashell;"|
| style="background: seashell;"|
|- style="background: seashell;"|
|rowspan=2|#1<br>△
|rowspan=2|[[File:Regular_polygon_30.svg|50px|{30}]]
|
|colspan=2|120-cell edge{{Efn|name=120-cell Petrie {30}-gon}}
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|{{red|<big>'''1'''</big>}}<br>1200{{Efn|name=120-cell characteristic rotation}}
|rowspan=2|{{blue|<big>'''4'''</big>}}<br>{3,3}
|- style="background: seashell;"|
|15.5~°
|{{radic|0.𝜀}}{{Efn|1=The fractional square root chord lengths are given as decimal fractions where:
{{indent|7}}𝚽 ≈ 0.618 is the inverse golden ratio <small>{{sfrac|1|φ}}</small>
{{indent|7}}𝚫 = 1 - 𝚽 = 𝚽<sup>2</sup> ≈ 0.382
{{indent|7}}𝜀 = {{radic|𝚫<sup>2</sup>/2}} ≈ 0.073<br>
and the 120-cell edge-length {{sfrac|1|φ<sup>2</sup>{{radic|2}}}} is:
{{indent|7}}𝛇 = {{radic|𝜀}} ≈ 0.270<br>
For example:
{{indent|7}}𝛇 = {{radic|0.𝜀}} = {{radic|0.073~}} ≈ 0.270|name=fractional square roots|group=}}
|0.270~
|- style="background: seashell;"|
|rowspan=2|#2<br><big>☐</big>
|rowspan=2|[[File:Regular_star_figure_2(15,1).svg|50px|{30/2}=2{15}]]
|{{^|1/φ{{radic|2}}}}
|colspan=2|face diagonal{{Efn|The #2 chord joins vertices which are 2 edge lengths apart: the vertices of the 120-cell's tetrahedral vertex figure, the second section of the 120-cell beginning with a vertex, denoted 1<sub>0</sub>. The #2 chords are the edges of this tetrahedron, and the #1 chords are its long radii. The #2 chords are also diagonal chords of the 120-cell's pentagon faces.{{Efn|The face [[Pentagon#Regular pentagons|pentagon diagonal]] (the #2 chord) is in the [[golden ratio]] φ ≈ 1.618 to the face pentagon edge (the 120-cell edge, the #1 chord).{{Efn|name=dodecahedral cell metrics}}|name=face pentagon chord}}|name=#2 chord}}
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>3600<br>
|rowspan=2|{{blue|<big>'''12'''</big>}}<br>2{3,4}
|- style="background: seashell;"|
|25.2~°
|{{radic|0.19~}}
|0.437~
|- style="background: yellow;"|
|rowspan=2|#3<br><big>✩</big>
|rowspan=2|[[File:Regular_star_figure_3(10,1).svg|50px|{30/3}=3{10}]]
|𝝅/5{{^|1/φ}}
|colspan=2|[[600-cell#Decagons|great decagon]] <math>\phi^{-1}</math>
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|{{green|<big>'''10'''</big>}}{{Efn|name=inscribed counts}}<br>720
|rowspan=2|
|rowspan=2|<br>7200
|rowspan=2|{{blue|<big>'''24'''</big>}}<br>2{3,5}
|- style="background: yellow;"|
|36°
|{{radic|0.𝚫}}
|0.618~
|- style="background: seashell;"|
|rowspan=2|#4<br>△
|rowspan=2|[[File:Regular_star_figure_2(15,2).svg|50px|{30/4}=2{15/2}]]
|{{Efn|name=irregular great dodecagon}}
|colspan=2|cell diameter{{Efn||name=dodecahedral cell metrics}}
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>1200
|rowspan=2|{{blue|<big>'''4'''</big>}}<br>{3,3}
|- style="background: seashell;"|
|44.5~°
|{{radic|0.57~}}
|0.757~
|- style="background: paleturquoise;"|
|rowspan=2|#5<br>△
|rowspan=2|[[File:Regular_star_figure_5(6,1).svg|50px|{30/5}=5{6}]]
|𝝅/3
|colspan=2|[[600-cell#Hexagons|great hexagon]]{{Efn|[[File:Regular_star_figure_5(6,1).svg|thumb|180px|[[Triacontagon#Triacontagram|Triacontagram {30/5}=5{6}]], the 120-cell's skew Petrie 30-gon as a compound of 5 great hexagons.]] Each great hexagon edge is the axis of a zig-zag of 5 120-cell edges. The 120-cell's Petrie polygon is a helical zig-zag of 30 120-cell edges, spiraling around a [[0-gon]] great circle axis that does not intersect any vertices.{{Efn|name=two coaxial Petrie 30-gons}} There are 5 great hexagons inscribed in each Petrie polygon, in five different central planes.{{Efn|name=same 200 planes}}|name=great hexagon}}
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>32
|rowspan=2|{{green|<big>'''225'''</big>}}{{Efn|name=inscribed counts}}<br>96
|rowspan=2|{{green|<big>'''225'''</big>}}<br><br>
|rowspan=2|{{red|<big>'''5'''</big>}}{{Efn|name=inscribed counts}}<br>1200
|rowspan=2|
|rowspan=2|<br>2400{{Efn|name=same 200 planes}}
|rowspan=2|{{blue|<big>'''32'''</big>}}<br>4{4,3}
|- style="background: paleturquoise;"|
|60°
|{{radic|1}}
|1
|- style="background: yellow;"|
|rowspan=2|#6<br><big>✩</big>
|rowspan=2|[[File:Regular_star_figure_6(5,1).svg|50px|{30/6}=6{5}]]
|2𝝅/5{{^|{{radic|3−φ}}}}
|colspan=2|[[600-cell#Decagons and 5𝝅 polygrams|great pentagon]]{{Efn|name=great pentagon}}
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>720
|rowspan=2|
|rowspan=2|<br>7200
|rowspan=2|{{blue|<big>'''24'''</big>}}<br>2{3,5}
|- style="background: yellow;"|
|72°
|{{radic|1.𝚫}}
|1.175~
|- style="background: paleturquoise;"|
|rowspan=2|#7<br><big>☐</big>
|rowspan=2|[[File:Regular_star_polygon_30-7.svg|50px|{30/7}]]
|𝝅/2
|colspan=2|[[600-cell#Squares|great square]]{{Efn|name=rays and bases}}
|rowspan=2|
|rowspan=2|{{green|<big>'''675'''</big>}}{{Efn|name=rays and bases}}<br>24
|rowspan=2|{{green|<big>'''675'''</big>}}<br>48
|rowspan=2|<br>72
|rowspan=2|
|rowspan=2|<br>1800
|rowspan=2|<br>
|rowspan=2|<br>16200
|rowspan=2|{{blue|<big>'''54'''</big>}}<br>9{3,4}
|- style="background: paleturquoise;"|
|90°
|{{radic|2}}
|1.414~
|- style="background: seashell;"|
|rowspan=2|#8<br>△
|rowspan=2|[[File:Regular_star_figure_2(15,4).svg|50px|{30/8}=2{15/4}]]
|
|colspan=2|[[5-cell#Boerdijk–Coxeter helix|5-cell]]{{Efn|The [[5-cell#Boerdijk–Coxeter helix|Petrie polygon of the 5-cell]] is the pentagon (5-gon), and the Petrie polygon of the 120-cell is the triacontagon (30-gon).{{Efn|name=120-cell Petrie {30}-gon}} Each 120-cell Petrie 30-gon lies completely orthogonal to six 5-cell Petrie 5-gons, which belong to six of the 120 disjoint regular 5-cells inscribed in the 120-cell.{{Efn|name=inscribed 5-cells}}|name=orthogonal Petrie polygons.}}
|rowspan=2|{{red|<big>'''120'''</big>}}{{Efn|name=inscribed 5-cells}}<br>10
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>720
|rowspan=2|<br>1200{{Efn|name=120-cell characteristic rotation}}
|rowspan=2|{{blue|<big>'''4'''</big>}}<br>{3,3}
|- style="background: seashell;"|
|104.5~°
|{{radic|2.5}}
|1.581~
|- style="background: yellow;"|
|rowspan=2|#9<br><big>✩</big>
|rowspan=2|[[File:Regular_star_figure_3(10,3).svg|50px|{30/9}=3{10/3}]]
|3𝝅/5
|colspan=2|[[golden section]] <math>\phi</math>
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>720
|rowspan=2|
|rowspan=2|<br>7200
|rowspan=2|{{blue|<big>'''24'''</big>}}<br>2{3,5}
|- style="background: yellow;"|
|108°
|{{radic|2.𝚽}}
|1.618~
|- style="background: paleturquoise;"|
|rowspan=2|#10<br>△
|rowspan=2|[[File:Regular_star_figure_10(3,1).svg|50px|{30/10}=10{3}]]
|2𝝅/3
|colspan=2|[[24-cell#Triangles|great triangle]]
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>32
|rowspan=2|{{red|<big>'''25'''</big>}}{{Efn|name=inscribed counts}}<br>96
|rowspan=2|
|rowspan=2|<br>1200
|rowspan=2|
|rowspan=2|<br>2400
|rowspan=2|{{blue|<big>'''32'''</big>}}<br>4{4,3}
|- style="background: paleturquoise;"|
|120°
|{{radic|3}}
|1.732~
|- style="background: seashell;"|
|rowspan=2|#11<br>△
|rowspan=2|[[File:Regular_star_polygon_30-11.svg|50px|{30/11}]]
|
|colspan=2|[[600-cell#Boerdijk–Coxeter helix rings|{30/11}-gram]]{{Efn|name={30/11}-gram}}
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>1200
|rowspan=2|{{blue|<big>'''4'''</big>}}<br>{3,3}
|- style="background: seashell;"|
|135.5~°
|{{radic|3.43~}}
|1.851~
|- style="background: yellow;"|
|rowspan=2|#12<br><big>✩</big>
|rowspan=2|[[File:Regular_star_figure_6(5,2).svg|50px|{30/12}=6{5/2}]]
|4𝝅/5{{^|{{radic|2+φ}}}}
|colspan=2|great [[Pentagon#Regular pentagons|pentagon diag]]
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>720
|rowspan=2|
|rowspan=2|<br>7200
|rowspan=2|{{blue|<big>'''24'''</big>}}<br>2{3,5}
|- style="background: yellow;"|
|144°{{Efn|name=dihedral}}
|{{radic|3.𝚽}}
|1.902~
|- style="background: seashell;"|
|rowspan=2|#13<br><big>☐</big>
|rowspan=2|[[File:Regular_star_polygon_30-13.svg|50px|{30/13}]]
|
|colspan=2|[[Triacontagon#Triacontagram|{30/13}-gram]]
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>3600<br>
|rowspan=2|{{blue|<big>'''12'''</big>}}<br>2{3,4}
|- style="background: seashell;"|
|154.8~°
|{{radic|3.81~}}
|1.952~
|- style="background: seashell;"|
|rowspan=2|#14<br>△
|rowspan=2|[[File:Regular_star_figure_2(15,7).svg|50px|{30/14}=2{15/7}]]
|
|colspan=2|[[Triacontagon#Triacontagram|{30/14}=2{15/7}]]
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|
|rowspan=2|<br>1200<br>
|rowspan=2|{{blue|<big>'''4'''</big>}}<br>{3,3}
|- style="background: seashell;"|
|164.5~°
|{{radic|3.93~}}
|1.982~
|- style="background: paleturquoise;"|
|rowspan=2|#15<br><small>△☐✩</small>
|rowspan=2|[[File:Regular_star_figure_15(2,1).svg|50px|30/15}=15{2}]]
|𝝅
|colspan=2|[[diameter]]
|rowspan=2|
|rowspan=2|{{red|<big>'''75'''</big>}}{{Efn|name=inscribed counts}}<br>4
|rowspan=2|<br>8
|rowspan=2|<br>12
|rowspan=2|<br>48
|rowspan=2|<br>60
|rowspan=2|<br>240
|rowspan=2|<br>300{{Efn|name=rays and bases}}
|rowspan=2|{{blue|<big>'''1'''</big>}}<br><br>
|- style="background: paleturquoise;"|
|180°
|{{radic|4}}
|2
|-
!colspan=5|Squared lengths total{{Efn|The sum of the squared lengths of all the distinct chords of any regular convex n-polytope of unit radius is the square of the number of vertices.{{Sfn|Copher|2019|loc=§3.2 Theorem 3.4|p=6}}}}
| style="background: seashell;"|25
| style="background: paleturquoise;"|64
| style="background: paleturquoise;"|256
| style="background: paleturquoise;"|576
| style="background: yellow;"|
| style="background: yellow;"|14400
| style="background: seashell;"|
| style="background: seashell;"|360000{{Efn|name=additional 120-cell chords}}
!<big>{{blue|'''300'''}}</big>
|}

[[File:15 major chords.png|thumb|300px|The major{{Efn|name=additional 120-cell chords}} chords #1 - #15 join vertex pairs which are 1 - 15 edges apart on a Petrie polygon.]]
The annotated chord table is a complete [[bill of materials]] for constructing the 120-cell. All of the 2-polytopes, 3-polytopes and 4-polytopes in the 120-cell are made from the 15 1-polytopes in the table.

The black integers in table cells are incidence counts of the row's chord in the column's 4-polytope. For example, in the '''#3''' chord row, the 600-cell's 72 great decagons contain 720 '''#3''' chords in all.

The '''{{red|red}}''' integers are the number of disjoint 4-polytopes above (the column label) which compounded form a 120-cell. For example, the 120-cell is a compound of <big>{{red|'''25'''}}</big> disjoint 24-cells (25 * 24 vertices = 600 vertices).

The '''{{green|green}}''' integers are the number of distinct 4-polytopes above (the column label) which can be picked out in the 120-cell. For example, the 120-cell contains <big>{{green|'''225'''}}</big> distinct 24-cells which share components.

The '''{{blue|blue}}''' integers in the right column are incidence counts of the row's chord at each 120-cell vertex. For example, in the '''#3''' chord row, <big>{{blue|'''24'''}}</big> '''#3''' chords converge at each of the 120-cell's 600 vertices, forming a double icosahedral [[vertex figure]] 2{3,5}. In total <big>{{blue|'''300'''}}</big> major chords{{Efn|name=additional 120-cell chords}} of 15 distinct lengths meet at each vertex of the 120-cell.

=== Relationships among interior polytopes ===
The 120-cell is the compound of all five of the other regular convex 4-polytopes. All the relationships among the regular 1-, 2-, 3- and 4-polytopes occur in the 120-cell.{{Efn|The 120-cell contains instances of all of the regular convex 1-polytopes, 2-polytopes, 3-polytopes and 4-polytopes, ''except'' for the regular polygons {7} and above, most of which do not occur. {10} is a notable exception which ''does'' occur. Various regular [[skew polygon]]s {7} and above occur in the 120-cell, notably {11},{{Efn|name={30/11}-gram}} {15}{{Efn|name=120-cell characteristic rotation}} and {30}.{{Efn|name=two coaxial Petrie 30-gons}}|name=elements}} It is a four-dimensional [[jigsaw puzzle]] in which all those polytopes are the parts.{{Sfn|Schleimer|Segerman|2013}} Although there are many sequences in which to construct the 120-cell by putting those parts together, ultimately they only fit together one way. The 120-cell is the unique solution to the combination of all these polytopes.{{Sfn|Stillwell|2001}}

The regular 1-polytope occurs in only [[#Chords|15 distinct lengths]] in any of the component polytopes of the 120-cell.{{Efn|name=additional 120-cell chords}}

Only 4 of those 15 chords occur in the 16-cell, 8-cell and 24-cell. The four {{background color|paleturquoise|[[24-cell#Hypercubic chords|hypercubic chords]]}} {{radic|1}}, {{radic|2}}, {{radic|3}} and {{radic|4}} are sufficient to build the 24-cell and all its component parts. The 24-cell is the unique solution to the combination of these 4 chords and all the regular polytopes that can be built from them.

{{see also|24-cell#Relationships among interior polytopes}}

An additional 4 of the 15 chords are required to build the 600-cell. The four {{background color|yellow|[[600-cell#Golden chords|golden chords]]}} are square roots of irrational fractions that are functions of {{radic|5}}. The 600-cell is the unique solution to the combination of these 8 chords and all the regular polytopes that can be built from them. Notable among the new parts found in the 600-cell which do not occur in the 24-cell are pentagons, and icosahedra.

{{see also|600-cell#Icosahedra}}

All 15 chords, and 15 other distinct chordal distances enumerated below, occur in the 120-cell. Notable among the new parts found in the 120-cell which do not occur in the 600-cell are regular 5-cells.{{Efn|Dodecahedra emerge as ''visible'' features in the 120-cell, but they also occur in the 600-cell as ''interior'' polytopes.{{Sfn|Coxeter|1973|p=298|loc=Table V: (iii) Sections of {3,3,5} beginning with a vertex}}}}
The relationships between the ''regular'' 5-cell (the [[simplex]] regular 4-polytope) and the other regular 4-polytopes are manifest directly only in the 120-cell.{{Efn|There is a geometric relationship between the regular 5-cell (4-simplex) and the regular 16-cell (4-orthoplex), but it is manifest only indirectly through the [[Tetrahedron|3-simplex]] and [[5-orthoplex]]. An [[simplex|<math>n</math>-simplex]] is bounded by <math>n+1</math> vertices and <math>n+1</math> (<math>n</math>-1)-simplex facets, and has <math>n+1</math> long diameters (its edges) of length <math>\sqrt{n+1}/\sqrt{n}</math> radii. An [[orthoplex|<math>n</math>-orthoplex]] is bounded by <math>2n</math> vertices and <math>2^n</math> (<math>n</math>-1)-simplex facets, and has <math>n</math> long diameters (its orthogonal axes) of length <math>2</math> radii. An [[hypercube|<math>n</math>-cube]] is bounded by <math>2^n</math> vertices and <math>2n</math> (<math>n</math>-1)-cube facets, and has <math>2^{n-1}</math> long diameters of length <math>\sqrt{n}</math> radii.{{Efn|The <math>n</math>-simplex's facets are larger than the <math>n</math>-orthoplex's facets. For <math>n=4</math>, the edge lengths of the 5-cell and 16-cell and 8-cell are in the ratio of <math>\sqrt{5}</math> to <math>\sqrt{4}</math> to <math>\sqrt{2}</math>.|name=root 5/root 4/root 2}} The <math>\sqrt{3}</math> long diameters of the 3-cube are shorter than the <math>\sqrt{4}</math> axes of the 3-orthoplex. The [[16-cell#Coordinates|coordinates of the 4-orthoplex]] are the permutations of <math>(0,0,0,\pm 1)</math>, and the 4-space coordinates of one of its 16 facets (a 3-simplex) are the permutations of <math>(0,0,0,1)</math>.{{Efn|Each 3-facet of the 4-orthoplex, a tetrahedron permuting <math>(0,0,0,1)</math>, and its completely orthogonal 3-facet permuting <math>(0,0,0,-1)</math>, comprise all 8 vertices of the 4-orthoplex. Uniquely, the 4-orthoplex is also the 4-[[demihypercube|demicube]], half the vertices of the 4-cube. This relationship among the 4-simplex, 4-orthoplex and 4-cube is unique to <math>n=4</math>. The 4-orthoplex's completely orthogonal 3-simplex facets are a pair of 3-demicubes which occupy alternate vertices of completely orthogonal 3-cubes in the same 4-cube. Projected orthogonally into the same 3-hyperplane, the two 3-facets would be two tetrahedra inscribed in the same 3-cube. (More generally, completely orthogonal polytopes are mirror reflections of each other.)|name=4-simplex-orthoplex-cube relation}} The <math>\sqrt{4}</math> long diameters of the 4-cube are the same length as the <math>\sqrt{4}</math> axes of the 4-orthoplex. The [[5-orthoplex#Cartesian coordinates|coordinates of the 5-orthoplex]] are the permutations of <math>(0,0,0,0,\pm 1)</math>, and the 5-space coordinates of one of its 32 facets (a 4-simplex) are the permutations of <math>(0,0,0,0,1)</math>.{{Efn|Each 4-facet of the 5-orthoplex, a 4-simplex (5-cell) permuting <math>(0,0,0,0,1)</math>, and its completely orthogonal 4-facet permuting <math>(0,0,0,0,-1)</math>, comprise all 10 vertices of the 5-orthoplex.}} The <math>\sqrt{5}</math> long diameters of the 5-cube are longer than the <math>\sqrt{4}</math> axes of the 5-orthoplex.|name=simplex-orthoplex-cube relation}} The 600-point 120-cell is a compound of 120 disjoint 5-point 5-cells, and it is also a compound of 5 disjoint 120-point 600-cells (two different ways). Each 5-cell has one vertex in each of 5 disjoint 600-cells, and therefore in each of 5 disjoint 24-cells, 5 disjoint 8-cells, and 5 disjoint 16-cells.{{Efn|No vertex pair of any of the 120 5-cells (no [[5-cell#Geodesics and rotations|great digon central plane of a 5-cell]]) occurs in any of the 675 16-cells (the 675 [[16-cell#Coordinates|Cartesian basis sets of 6 orthogonal central planes]]).{{Efn|name=rays and bases}}}} Each 5-cell is a ring (two different ways) joining 5 disjoint instances of each of the other regular 4-polytopes.{{Efn|name=distinct circuits of the 5-cell}}

{{see also|5-cell#Geodesics and rotations}}

=== Geodesic rectangles ===
The 30 distinct chords{{Efn|name=additional 120-cell chords}} found in the 120-cell occur as 15 pairs of 180° complements. They form 15 distinct kinds of great circle polygon that lie in central planes of several kinds: {{Backgroundcolor|palegreen|△ planes that intersect {12} vertices}} in an irregular dodecagon,{{Efn|name=irregular great dodecagon}} {{Backgroundcolor|yellow|✩ planes that intersect {10} vertices}} in a regular decagon, and {{Backgroundcolor|gainsboro|☐ planes that intersect {4} vertices}} in several kinds of rectangle, including a square. 

Each great circle polygon is characterized by its pair of 180° complementary chords. The chord pairs form great circle polygons with parallel opposing edges, so each great polygon is either a rectangle or a compound of a rectangle, with the two chords as the rectangle's edges.

Each of the 15 complementary chord pairs corresponds to a distinct pair of opposing [[#Concentric hulls|polyhedral sections]] of the 120-cell, beginning with a vertex, the 0<sub>0</sub> section. The correspondence is that each 120-cell vertex is surrounded by each polyhedral section's vertices at a uniform distance (the chord length), the way a polyhedron's vertices surround its center at the distance of its long radius.{{Efn|In the curved 3-dimensional space of the 120-cell's surface, each of the 600 vertices is surrounded by 15 pairs of polyhedral sections, each section at the "radial" distance of one of the 30 distinct chords. The vertex is not actually at the center of the polyhedron, because it is displaced in the fourth dimension out of the section's hyperplane, so that the ''apex'' vertex and its surrounding ''base'' polyhedron form a [[polyhedral pyramid]]. The characteristic chord is radial around the apex, as the pyramid's lateral edges.}} The #1 chord is the "radius" of the 1<sub>0</sub> section, the tetrahedral vertex figure of the 120-cell.{{Efn|name=#2 chord}} The #14 chord is the "radius" of its congruent opposing 29<sub>0</sub> section. The #7 chord is the "radius" of the central section of the 120-cell, in which two opposing 15<sub>0</sub> sections are coincident.

{| class=wikitable style="white-space:nowrap;text-align:center"
!colspan=13|30 chords (15 180° pairs) make 15 kinds of great circle polygons and polyhedral sections{{Sfn|Coxeter|1973|pp=300-301|loc=Table V:(v) Simplified sections of {5,3,3} (edge 2φ<sup>−2</sup>√2 [radius 4]) beginning with a vertex; Coxeter's table lists 16 non-point sections labelled 1<sub>0</sub> − 16<sub>0</sub>|ps=, but 14<sub>0</sub> and 16<sub>0</sub> are congruent opposing sections and 15<sub>0</sub> opposes itself; there are 29 non-point sections, denoted 1<sub>0</sub> − 29<sub>0</sub>, in 15 opposing pairs.}}
|-
!colspan=4|Short chord
!colspan=2|Great circle polygons
!Rotation
!colspan=4|Long chord
|- style="background: palegreen;"|
|rowspan=2|1<sub>0</sub><br><br>#1
|{{Efn|In the 120-cell's isoclinic rotations the rotation arc-angle is 12° (1/30 of a circle), not the 15.5~° arc of the #1 edge chord. Regardless of which central planes are the invariant rotation planes, any 120-cell isoclinic rotation by 12° will take the great polygon in ''every'' central plane to a congruent great polygon in a Clifford parallel central plane that is 12° away. Adjacent Clifford parallel great polygons (of every kind) are completely disjoint, and their nearest vertices are connected by ''two'' 120-cell edges (#1 chords of arc-length 15.5~°). The 12° rotation angle is not the arc of any vertex-to-vertex chord in the 120-cell. It occurs only as the two equal angles between adjacent Clifford parallel central ''planes'',{{Efn|name=isoclinic}} and it is the separation between adjacent rotation planes in ''all'' the 120-cell's various isoclinic rotations (not only in its characteristic rotation).|name=12° rotation angle}}
|colspan=2|<math>1 / \phi^2\sqrt{2}</math>
|rowspan=2|[[File:Irregular great hexagons of the 120-cell.png|100px]]
|rowspan=2|400 irregular great hexagons{{Efn|name=irregular great dodecagon}} / 4<br>
(600 great rectangles)<br>
in 200 △ planes
|rowspan=2|4𝝅{{Efn|name=isocline circumference}}<br>[[Triacontagon#Triacontagram|{15/4}]]{{Efn|name=120-cell characteristic rotation}}<br>#4{{Efn|The characteristic isoclinic rotation of the 120-cell, in the invariant planes in which its edges (#1 chords) lie, takes those edges to similar edges in Clifford parallel central planes. Since an isoclinic rotation{{Efn|name=isoclinic rotation}} is a double rotation (in two completely orthogonal invariant central planes at once), in each incremental rotation step from vertex to neighboring vertex the vertices travel between central planes on helical great circle isoclines, not on ordinary great circles,{{Efn|name=isocline}} over an isocline chord which in this particular rotation is a #4 chord of 44.5~° arc-length.{{Efn|The isocline chord of the 120-cell's characteristic rotation{{Efn|name=120-cell characteristic rotation}} is the #4 chord of 44.5~° arc-angle (the larger edge of the irregular great dodecagon), because in that isoclinic rotation by two equal 12° rotation angles{{Efn|name=12° rotation angle}} each vertex moves to another vertex 4 edge-lengths away on a Petrie polygon, and the circular geodesic path it rotates on (its isocline){{Efn|name=isocline}} does not intersect any nearer vertices.{{^|The #2 chords join vertices which are 2 edge lengths apart,{{Efn|name=#2 chord}} as do the ''isocline'' chords of other characteristic isoclinic rotations whose edge chords are their rotation chords.{{Efn|name=characteristic rotation}} The #4 chords join vertices which are 4 edge lengths apart.{{Efn|The #4 chord is {{radic|3}} times the #2 chord,{{Efn|name=#2 chord}} the same relationship the #10 {{radic|3}} isocline chord has to its #5 {{radic|1}} rotation chord, because the invariant planes of two different characteristic rotations (the 120-cell's irregular great hexagons and the 24-cell's regular hexagons, respectively) both have sets of invariant rotation planes which are distinct subsets of the same 200 △ dodecagon central planes.{{Efn|name=irregular great dodecagon}} The similar proportion of these two chord pairs is because of the similarity of the two rotations that take place in the same rotation planes (but notice that the #2 rotation chords do not lie in those △ dodecagon planes). They have a 3 in 1 relation, in that the #1 edge and its #4 isocline chord sum to 60°, as the 60° edge and its 120° chord sum to 180°.|name=regular and irregular great hexagon isoclinic rotations}} The #2 rotation chord is the total vertex displacement as measured in the moving reference frame of one of the invariant planes, the way the #4 isocline chord is the total vertex displacement as measured in the stationary reference frame.|name=#2 and #4 chords}}|name=120-cell rotation angle}}|name=#4 isocline chord}}
|
|colspan=2|<math>\phi^{5}\sqrt{3} / \sqrt{8}</math>
|rowspan=2|29<sub>0</sub><br><br>#14
|- style="background: palegreen;"|
|15.5~°
|{{radic|0.𝜀}}{{Efn|name=fractional square roots}}
|0.270~
|164.5~°
|{{radic|3.93~}}
|1.982~
|- style="background: gainsboro;"|
|rowspan=2|2<sub>0</sub><br><br>#2
|{{Efn|name=#2 chord}}
|colspan=2|<math>1 / \phi\sqrt{2}</math>
|rowspan=2|[[File:25.2° × 154.8° chords great rectangle.png|100px]]
|rowspan=2|Great rectangles<br>in <big>☐</big> planes
|rowspan=2|4𝝅<br>[[Triacontagon#Triacontagram|{30/13}]]<br>#13
|
|colspan=2|
|rowspan=2|28<sub>0</sub><br><br>#13
|- style="background: gainsboro;"|
|25.2~°
|{{radic|0.19~}}
|0.437~
|154.8~°
|{{radic|3.81~}}
|1.952~
|- style="background: yellow;"|
|rowspan=2|3<sub>0</sub><br><br>#3
|<math>\pi / 5</math>
|colspan=2|<math>1 / \phi</math>
|rowspan=2|[[File:Great decagon rectangle.png|100px]]
|rowspan=2|720 great decagons / 12<br>(3600 great rectangles)<br>in 720 <big>✩</big> planes
|rowspan=2|5𝝅<br>[[600-cell#Decagons and 5𝝅 polygrams|{15/2}]]<br>#5
|<math>4\pi / 5</math>
|colspan=2|<math>\sqrt{2+\phi}</math>
|rowspan=2|27<sub>0</sub><br><br>#12
|- style="background: yellow;"|
|36°
|{{radic|0.𝚫}}
|0.618~
|144°{{Efn|name=dihedral}}
|{{radic|3.𝚽}}
|1.902~
|- style="background: gainsboro;"|
|rowspan=2|4<sub>0</sub><br><br>#4−1
|
|colspan=2|<math>\sqrt{1}/\sqrt{2}</math>
|rowspan=2|[[File:√0.5 × √3.5 great rectangle.png|100px]]
|rowspan=2|Great rectangles<br>in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|<math>\sqrt{7} / \sqrt{2}</math>
|rowspan=2|26<sub>0</sub><br><br>#11+1
|- style="background: gainsboro;"|
|41.4~°
|{{radic|0.5}}
|0.707~
|138.6~°
|{{radic|3.5}}
|1.871~
|- style="background: palegreen;"|
|rowspan=2|5<sub>0</sub><br><br>#4
|{{^|Efn|name=regular and irregular great hexagon isoclinic rotations}}
|colspan=2|<math>\sqrt{3} / \phi\sqrt{2}</math>
|rowspan=2|[[File:Irregular great dodecagon.png|100px]]
|rowspan=2|200 irregular great dodecagons{{Efn|This illustration shows just one of three related irregular great dodecagons that lie in three distinct △ central planes. Two of them (not shown) lie in Clifford parallel (disjoint) dodecagon planes, and share no vertices. The {{Color|blue}} central rectangle of #4 and #11 edges lies in a third dodecagon plane, not Clifford parallel to either of the two disjoint dodecagon planes and intersecting them both; it shares two vertices (a {{radic|4}} axis of the rectangle) with each of them. Each dodecagon plane contains two irregular great hexagons in alternate positions (not shown).{{Efn|name=irregular great dodecagon}} Thus each #4 chord of the great rectangle shown is a bridge between two Clifford parallel irregular great hexagons that lie in the two dodecagon planes which are not shown.{{Efn|Isoclinic rotations take Clifford parallel planes to each other, as planes of rotation tilt sideways like coins flipping.{{Efn|name=isoclinic rotation}} The #4 chord{{Efn|name=#4 isocline chord}} bridge is significant in an isoclinic rotation in ''regular'' great hexagons (the [[600-cell#Hexagons|24-cell's characteristic rotation]]), in which the invariant rotation planes are a subset of the same 200 dodecagon central planes as the 120-cell's characteristic rotation (in ''irregular'' great hexagons).{{Efn|name=120-cell characteristic rotation}} In each 12° arc{{Efn|name=120-cell rotation angle}} of the 24-cell's characteristic rotation of the 120-cell, every ''regular'' great hexagon vertex is displaced to another vertex, in a Clifford parallel regular great hexagon that is a #4 chord away. Adjacent Clifford parallel regular great hexagons have six pairs of corresponding vertices joined by #4 chords. The six #4 chords are edges of six distinct great rectangles in six disjoint dodecagon central planes which are mutually Clifford parallel.|name=#4 isocline chord bridge}}|name=dodecagon rotation}} / 4<br>(600 great rectangles)<br>in 200 △ planes
|rowspan=2|{{Efn|name=#4 isocline chord bridge}}
|
|colspan=2|<math>\phi^2 / \sqrt{2}</math>
|rowspan=2|25<sub>0</sub><br><br>#11
|- style="background: palegreen;"|
|44.5~°
|{{radic|0.57~}}
|0.757~
|135.5~°
|{{radic|3.43~}}
|1.851~
|- style="background: gainsboro; height:50px"|
|rowspan=2|6<sub>0</sub><br><br>#4+1
|{{^|<math>\pi / 3.67\sim</math>}}
|colspan=2|
|rowspan=2|[[File:49.1° × 130.9° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br>in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|24<sub>0</sub><br><br>#11−1
|- style="background: gainsboro;"|
|49.1~°
|{{radic|0.69~}}
|0.831~
|130.9~°
|{{radic|3.31~}}
|1.819~
|- style="background: gainsboro; height:50px"|
|rowspan=2|7<sub>0</sub><br><br>#5−1
|{{^|<math>\pi / 3.21\sim</math>}}
|colspan=2|
|rowspan=2|[[File:56° × 124° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br>in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|23<sub>0</sub><br><br>#10+1
|- style="background: gainsboro;"|
|56°
|{{radic|0.88~}}
|0.939~
|124°
|{{radic|3.12~}}
|1.766~
|- style="background: palegreen;"|
|rowspan=2|8<sub>0</sub><br><br>#5
|<math>\pi / 3</math>
|colspan=2|
|rowspan=2|[[File:Great hexagon.png|100px]]
|rowspan=2|400 regular [[600-cell#Hexagons|great hexagons]]{{Efn|name=great hexagon}} / 16<br> (1200 great rectangles)<br>in 200 △ planes
|rowspan=2|4𝝅{{Efn|All 3-sphere isoclines of the same circumference are directly congruent circles. An ordinary great circle is an isocline of circumference <math>2\pi r</math>; simple rotations of unit-radius polytopes take place on 2𝝅 isoclines. Double rotations may have isoclines of other than <math>2\pi r</math> circumference. The ''characteristic rotation'' of a regular 4-polytope is the isoclinic rotation in which the central planes containing its edges are invariant planes of rotation. The 16-cell and 24-cell edge-rotate on isoclines of 4𝝅 circumference. The 600-cell edge-rotates on isoclines of 5𝝅 circumference.|name=isocline circumference}}<br>[[600-cell#Hexagons and 4𝝅 polygrams|2{10/3}]]<br>#4
|<math>2\pi / 3</math>
|colspan=2|
|rowspan=2|22<sub>0</sub><br><br>#10
|- style="background: palegreen;"|
|60°
|{{radic|1}}
|1
|120°
|{{radic|3}}
|1.732~
|- style="background: gainsboro; height:50px"|
|rowspan=2|9<sub>0</sub><br><br>#5+1
|{{^|<math>\pi / 2.72\sim</math>}}
|colspan=2|
|rowspan=2|[[File:66.1° × 113.9° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br> in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|21<sub>0</sub><br><br>#10−1
|- style="background: gainsboro;"|
|66.1~°
|{{radic|1.19~}}
|1.091~
|113.9~°
|{{radic|2.81~}}
|1.676~
|- style="background: gainsboro; height:50px"|
|rowspan=2|10<sub>0</sub><br><br>#6−1
|{{^|<math>\pi / 2.58\sim</math>}}
|colspan=2|
|rowspan=2|[[File:69.8° × 110.2° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br> in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|20<sub>0</sub><br><br>#9+1
|- style="background: gainsboro;"|
|69.8~°
|{{radic|1.31~}}
|1.144~
|110.2~°
|{{radic|2.69~}}
|1.640~
|- style="background: yellow;"|
|rowspan=2|11<sub>0</sub><br><br>#6
|<math>2\pi/5</math>
|colspan=2|<math>\sqrt{3-\phi}</math>
|rowspan=2|[[File:Great pentagons rectangle.png|100px]]
|rowspan=2|1440 [[600-cell#Decagons and 5𝝅 polygrams|great pentagons]]{{Efn|name=great pentagon}} / 12<br>(3600 great rectangles)<br>
in 720 <big>✩</big> planes
|rowspan=2|4𝝅<br>[[600-cell#Squares and 4𝝅 polygrams|{24/5}]]<br>#9
|<math>3\pi / 5</math>
|colspan=2|<math>\phi</math>
|rowspan=2|19<sub>0</sub><br><br>#9
|- style="background: yellow;"|
|72°
|{{radic|1.𝚫}}
|1.175~
|108°
|{{radic|2.𝚽}}
|1.618~
|- style="background: palegreen; height:50px"|
|rowspan=2|12<sub>0</sub><br><br>#6+1
|{{^|<math>\pi/2.38\sim</math>}}
|colspan=2|<math>\sqrt{3} / \sqrt{2}</math>
|rowspan=2|[[File:Great 5-cell digons rectangle.png|100px]]
|rowspan=2|1200 [[5-cell#Geodesics and rotations|great digon 5-cell edges]]{{Efn|The [[5-cell#Geodesics and rotations|regular 5-cell has only digon central planes]] intersecting two vertices. The 120-cell with 120 inscribed regular 5-cells contains great rectangles whose longer edges are these digons, the edges of inscribed 5-cells of length {{radic|2.5}}. Three disjoint rectangles occur in one {12} central plane, where the six #8 {{radic|2.5}} chords belong to six disjoint 5-cells. The 12<sub>0</sub> sections and 18<sub>0</sub> sections are regular tetrahedra of edge length {{radic|2.5}}, the cells of regular 5-cells. The regular 5-cells' ten triangle faces lie in those sections; each of a face's three {{radic|2.5}} edges lies in a different {12} central plane.|name=5-cell rotation}} / 4<br>(600 great rectangles)<br>
in 200 △ planes
|rowspan=2|4𝝅{{Efn|name=isocline circumference}}<br>[[Pentagram|{5/2}]]<br>#8
|
|colspan=2|<math>\sqrt{5} / \sqrt{2}</math>
|rowspan=2|18<sub>0</sub><br><br>#8
|- style="background: palegreen;"|
|75.5~°
|{{radic|1.5}}
|1.224~
|104.5~°
|{{radic|2.5}}
|1.581~
|- style="background: gainsboro; height:50px"|
|rowspan=2|13<sub>0</sub><br><br>#6+2
|{{^|<math>\pi / 2.22\sim</math>}}
|colspan=2|
|rowspan=2|[[File:81.1° × 98.9° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br> in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|17<sub>0</sub><br><br>#8−1
|- style="background: gainsboro;"|
|81.1~°
|{{radic|1.69~}}
|1.300~
|98.9~°
|{{radic|2.31~}}
|1.520~
|- style="background: gainsboro; height:50px"|
|rowspan=2|14<sub>0</sub><br><br>#7−1
|{{^|<math>\pi / 2.13\sim</math>}}
|colspan=2|
|rowspan=2|[[File:84.5° × 95.5° great rectangle.png|100px]]
|rowspan=2|Great rectangles<br> in <big>☐</big> planes
|rowspan=2|
|
|colspan=2|
|rowspan=2|16<sub>0</sub><br><br>#7+1
|- style="background: gainsboro;"|
|84.5~°
|{{radic|0.81~}}
|1.345~
|95.5~°
|{{radic|2.19~}}
|1.480~
|- style="background: gainsboro;"|
|rowspan=2|15<sub>0</sub><br><br>#7
|<math>\pi / 2</math>
|colspan=2|
|rowspan=2|[[File:Great square rectangle.png|100px]]
|rowspan=2|4050 [[600-cell#Squares|great squares]]{{Efn|name=rays and bases}} / 27<br>
in 4050 <big>☐</big> planes
|rowspan=2|4𝝅<br>[[30-gon#Triacontagram|{30/7}]]<br>#7
|<math>\pi / 2</math>
|colspan=2|
|rowspan=2|15<sub>0</sub><br><br>#7
|- style="background: gainsboro;"|
|90°
|{{radic|2}}
|1.414~
|90°
|{{radic|2}}
|1.414~
|}

Each kind of great circle polygon (each distinct pair of 180° complementary chords) plays a role in a discrete isoclinic rotation{{Efn|An isoclinic{{Efn|name=isoclinic}} rotation is an equi-rotation-angled [[SO(4)#Double rotations|double rotation]] in two completely orthogonal invariant central planes of rotation at the same time. Every discrete isoclinic rotation has two characteristic arc-angles (chord lengths), its ''rotation angle'' and its ''isocline angle''.{{Efn|name=characteristic rotation}} In each incremental rotation step from vertex to neighboring vertex, each invariant rotation plane rotates by the rotation angle, and also tilts sideways (like a coin flipping) by an equal rotation angle.{{Efn|In an ''isoclinic'' rotation each invariant plane is Clifford parallel to the plane it moves to, and they do not intersect at any time (except at the central point). In a ''simple'' rotation the invariant plane intersects the plane it moves to in a line, and moves to it by rotating around that line.|name=plane movement in rotations}} Thus each vertex rotates on a great circle by one rotation angle increment, while simultaneously the whole great circle rotates with the completely orthogonal great circle by an equal rotation angle increment.{{Efn|It is easiest to visualize this ''incorrectly'', because the completely orthogonal great circles are Clifford parallel and do not intersect (except at the central point). Neither do the invariant plane and the plane it moves to. An invariant plane tilts sideways in an orthogonal central plane which is not its ''completely'' orthogonal plane, but Clifford parallel to it. It rotates ''with'' its completely orthogonal plane, but not ''in'' it. It is Clifford parallel to its completely orthogonal plane ''and'' to the plane it is moving to, and does not intersect them; the plane that it rotates ''in'' is orthogonal to all these planes and intersects them all.{{Efn|The plane in which an entire invariant plane rotates (tilts sideways) is (incompletely) orthogonal to both completely orthogonal invariant planes, and also Clifford parallel to both of them.{{Efn|Although perpendicular and linked (like adjacent links in a taught chain), completely orthogonal great polygons are also parallel, and lie exactly opposite each other in the 4-polytope, in planes that do not intersect except at one point, the common center of the two linked circles.|name=perpendicular and parallel}}}} In the 120-cell's characteristic rotation,{{Efn|name=120-cell characteristic rotation}} each invariant rotation plane is Clifford parallel to its completely orthogonal plane, but not adjacent to it; it reaches some other (nearest) parallel plane first. But if the isoclinic rotation taking it through successive Clifford parallel planes is continued through 90°, the vertices will have moved 180° and the tilting rotation plane will reach its (original) completely orthogonal plane.{{Efn|The 90 degree isoclinic rotation of two completely orthogonal planes takes them to each other. In such a rotation of a rigid 4-polytope, [[16-cell#Rotations|all 6 orthogonal planes]] rotate by 90 degrees, and also tilt sideways by 90 degrees to their completely orthogonal (Clifford parallel) plane.{{Sfn|Kim|Rote|2016|pp=8-10|loc=Relations to Clifford Parallelism}} The corresponding vertices of the two completely orthogonal great polygons are {{radic|4}} (180°) apart; the great polygons (Clifford parallel polytopes) are {{radic|4}} (180°) apart; but the two completely orthogonal ''planes'' are 90° apart, in the ''two'' orthogonal angles that separate them.{{Efn|name=isoclinic}} If the isoclinic rotation is continued through another 90°, each vertex completes a 360° rotation and each great polygon returns to its original plane, but in a different [[Orientation entanglement|orientation]] (axes swapped): it has been turned "upside down" on the surface of the 4-polytope (which is now "inside out"). Continuing through a second 360° isoclinic rotation (through four 90° by 90° isoclinic steps, a 720° rotation) returns everything to its original place and orientation.|name=exchange of completely orthogonal planes}}|name=rotating with the completely orthogonal rotation plane}} The product of these two simultaneous and equal great circle rotation increments is an overall displacement of each vertex by the isocline angle increment (the isocline chord length). Thus the rotation angle measures the vertex displacement in the reference frame of a moving great circle, and also the sideways displacement of the moving great circle (the distance between the great circle polygon and the adjacent Clifford parallel great circle polygon the rotation takes it to) in the stationary reference frame. The isocline chord length is the total vertex displacement in the stationary reference frame, which is an oblique chord between the two adjacent great circle polygons (the distance between their corresponding vertices in the rotation).|name=isoclinic rotation}} of a distinct class,{{Efn|Every class of discrete isoclinic rotation{{Efn|name=isoclinic rotation}} is characterized by its rotation and isocline angles and by which set of Clifford parallel central planes are its invariant planes of rotation. The '''characteristic isoclinic rotation of a 4-polytope''' is the class of discrete isoclinic rotation in which the set of invariant rotation planes contains the 4-polytope's edges; there is a distinct left (and right) rotation for each such set of Clifford parallel central planes (each [[Hopf fibration]] of the edge planes). If the edges of the 4-polytope form regular great circles, the rotation angle of the characteristic rotation is simply the edge arc-angle (the edge chord is simply the rotation chord). But in a regular 4-polytope with a tetrahedral vertex figure{{Efn|name=non-planar geodesic circle}} the edges do not form regular great circles, they form irregular great circles in combination with another chord. For example, the #1 chord edges of the 120-cell are edges of an irregular great dodecagon which also has #4 chord edges.{{Efn|name=irregular great dodecagon}} In such a 4-polytope, the rotation angle is not the edge arc-angle; in fact it is not necessarily the arc of any vertex chord.{{Efn|name=12° rotation angle}}|name=characteristic rotation}} which takes its great rectangle edges to similar edges in Clifford parallel great polygons of the same kind.{{Efn|In the 120-cell, completely orthogonal to every great circle polygon lies another great circle polygon of the same kind. The set of Clifford parallel invariant planes of a distinct isoclinic rotation is a set of such completely orthogonal pairs.{{Efn|name=Clifford parallel invariant planes}}}} There is a distinct left and right rotation of this class for each fiber bundle of Clifford parallel great circle polygons in the invariant planes of the rotation.{{Efn|Each kind of rotation plane has its characteristic fibration divisor, denoting the number of fiber bundles of Clifford parallel great circle polygons (of each distinct kind) that are found in rotation planes of that kind. Each bundle covers all the vertices of the 120-cell exactly once, so the total number of vertices in the great circle polygons of one kind, divided by the number of bundles, is always 600, the number of distinct vertices. For example, "400 irregular great hexagons / 4".}} In each class of rotation,{{Efn|[[Rotations in 4-dimensional Euclidean space]] are defined by at least one pair of completely orthogonal{{Efn|name=perpendicular and parallel}} central planes of rotation which are ''invariant'', which means that all points in the plane stay in the plane as the plane moves. A distinct left (and right) isoclinic{{Efn|name=isoclinic}} rotation may have multiple pairs of completely orthogonal invariant planes, and all those invariant planes are mutually [[Clifford parallel]]. A distinct class of discrete isoclinic rotation has a characteristic kind of great polygon in its invariant planes.{{Efn|name=characteristic rotation}} It has multiple distinct left (and right) rotation instances called ''fibrations'', which have disjoint sets of invariant rotation planes. The fibrations are disjoint bundles of Clifford parallel circular ''fibers'', the great circle polygons in their invariant planes.|name=Clifford parallel invariant planes}} vertices rotate on a distinct kind of circular geodesic isocline{{Efn|name=isocline}} which has a characteristic circumference, skew Clifford polygram{{Efn|name=Clifford polygon}} and chord number, listed in the Rotation column above.{{Efn|The 120-cell has 7200 distinct rotational displacements, each with its invariant rotation plane. The 7200 distinct central planes can be grouped into the sets of Clifford parallel invariant rotation planes of 25 distinct classes of (double) rotations, and are usually given as those sets.{{Sfn|Mamone|Pileio|Levitt|2010|loc=§4.5 Regular Convex 4-Polytopes, Table 2}}|name=distinct rotations}}

===Concentric hulls===
[[File:120-Cell showing the individual 8 concentric hulls and in combination.svg|thumb|left|640px|
Orthogonal projection of the 120-cell using any 3 of these Cartesian coordinate dimensions forms an outer hull of a [[Chamfered dodecahedron]] of Norm={{radic|8}}.<br />
Hulls 1, 2, & 7 are each overlapping pairs of [[Dodecahedron]]s.<br />
Hull 3 is a pair of [[Icosidodecahedron]]s.<br />
Hulls 4 & 5 are each pairs of [[Truncated icosahedron]]s.<br />
Hulls 6 & 8 are pairs of [[Rhombicosidodecahedron]]s.]]
{{Clear}}

===Polyhedral graph===
Considering the [[adjacency matrix]] of the vertices representing the polyhedral graph of the unit-radius 120-cell, the [[graph diameter]] is 15, connecting each vertex to its coordinate-negation at a [[Euclidean distance]] of 2 away (its circumdiameter), and there are 24 different paths to connect them along the polytope edges. From each vertex, there are 4 vertices at distance 1, 12 at distance 2, 24 at distance 3, 36 at distance 4, 52 at distance 5, 68 at distance 6, 76 at distance 7, 78 at distance 8, 72 at distance 9, 64 at distance 10, 56 at distance 11, 40 at distance 12, 12 at distance 13, 4 at distance 14, and 1 at distance 15. The adjacency matrix has 27 distinct eigenvalues ranging from {{sfrac|1|φ<sup>2</sup>{{radic|2}}}} ≈ 0.270, with a multiplicity of 4, to 2, with a multiplicity of 1. The multiplicity of eigenvalue 0 is 18, and the rank of the adjacency matrix is 582.

The vertices of the 120-cell polyhedral graph are [[vertex coloring|3-colorable]].

The graph is [[Eulerian path|Eulerian]] having degree 4 in every vertex. Its edge set can be decomposed into two [[hamiltonian path|Hamiltonian cycles]].<ref>{{cite book| author = Carlo H. Séquin | title = Symmetrical Hamiltonian manifolds on regular 3D and 4D polytopes | date = July 2005 | pages = 463–472 | publisher = Mathartfun.com | isbn = 9780966520163 | url = https://archive.bridgesmathart.org/2005/bridges2005-463.html#gsc.tab=0 | access-date=March 13, 2023}}</ref>

=== Constructions ===
The 120-cell is the sixth in the sequence of 6 convex regular 4-polytopes (in order of size and complexity).{{Efn|name=polytopes ordered by size and complexity}} It can be deconstructed into ten distinct instances (or five disjoint instances) of its predecessor (and dual) the [[600-cell]],{{Efn|name=2 ways to get 5 disjoint 600-cells}} just as the 600-cell can be deconstructed into twenty-five distinct instances (or five disjoint instances) of its predecessor the [[24-cell]],{{Efn|In the 120-cell, each 24-cell belongs to two different 600-cells.{{Sfn|van Ittersum|2020|p=435|loc=§4.3.5 The two 600-cells circumscribing a 24-cell}} The 120-cell contains 225 distinct 24-cells and can be partitioned into 25 disjoint 24-cells, so it is the convex hull of a compound of 25 24-cells.{{Sfn|Denney|Hooker|Johnson|Robinson|2020|p=5|loc=§2 The Labeling of H4}}|name=two 600-cells share a 24-cell}} the 24-cell can be deconstructed into three distinct instances of its predecessor the [[tesseract]] (8-cell), and the 8-cell can be deconstructed into two disjoint instances of its predecessor (and dual) the [[16-cell]].{{Sfn|Coxeter|1973|p=305|loc=Table VII: Regular Compounds in Four Dimensions}} The 120-cell contains 675 distinct instances (75 disjoint instances) of the 16-cell.{{Efn|The 120-cell has 600 vertices distributed symmetrically on the surface of a 3-sphere in four-dimensional Euclidean space. The vertices come in antipodal pairs, and the lines through antipodal pairs of vertices define the 300 '''rays''' [or axes] of the 120-cell. We will term any set of four mutually orthogonal rays (or directions) a '''[[Orthonormal basis|basis]]'''. The 300 rays form 675 bases, with each ray occurring in 9 bases and being orthogonal to its 27 distinct companions in these bases and to no other rays. The rays and bases constitute a [[Configuration (geometry)|geometric configuration]], which in the language of configurations is written as 300<sub>9</sub>675<sub>4</sub> to indicate that each ray belongs to 9 bases, and each basis contains 4 rays.{{Sfn|Waegell|Aravind|2014|loc=§2 Geometry of the 120-cell: rays and bases|pp=3-4}} Each basis corresponds to a distinct [[16-cell#Coordinates|16-cell]] containing four orthogonal axes and six orthogonal great squares. 75 completely disjoint 16-cells containing all 600 vertices of the 120-cell can be selected from the 675 distinct 16-cells.{{Efn|name=rotated 4-simplexes are completely disjoint}}|name=rays and bases}}

The reverse procedure to construct each of these from an instance of its predecessor preserves the radius of the predecessor, but generally produces a successor with a smaller edge length. The 600-cell's edge length is ~0.618 times its radius (the inverse [[golden ratio]]), but the 120-cell's edge length is ~0.270 times its radius.

==== Dual 600-cells ====
[[File:Chiroicosahedron-in-dodecahedron.png|thumb|150px|right|Five tetrahedra inscribed in a dodecahedron. Five opposing tetrahedra (not shown) can also be inscribed.]]

Since the 120-cell is the dual of the 600-cell, it can be constructed from the 600-cell by placing its 600 vertices at the center of volume of each of the 600 tetrahedral cells. From a 600-cell of unit long radius, this results in a 120-cell of slightly smaller long radius ({{sfrac|φ<sup>2</sup>|{{radic|8}}}} ≈ 0.926) and edge length of exactly 1/4. Thus the unit edge-length 120-cell (with long radius φ<sup>2</sup>{{radic|2}} ≈ 3.702) can be constructed in this manner just inside a 600-cell of long radius 4. The [[#Unit radius coordinates|unit radius 120-cell]] (with edge-length {{sfrac|1|φ<sup>2</sup>{{radic|2}}}} ≈ 0.270) can be constructed in this manner just inside a 600-cell of long radius {{sfrac|{{radic|8}}|φ<sup>2</sup>}} ≈ 1.080.

[[File:Dodecahedron_vertices.svg|thumb|150px|right|One of the five distinct cubes inscribed in the dodecahedron (dashed lines). Two opposing tetrahedra (not shown) lie inscribed in each cube, so ten distinct tetrahedra (one from each 600-cell in the 120-cell) are inscribed in the dodecahedron.{{Efn|In the [[120-cell#Dual 600-cells|dodecahedral cell]] of the unit-radius 120-cell, the length of the edge (the '''#1 [[#Chords|chord]]''' of the 120-cell) is {{sfrac|1|φ<sup>2</sup>{{radic|2}}}} ≈ 0.270. Eight {{Color|orange}} vertices lie at the Cartesian coordinates (±φ<sup>3</sup>{{radic|8}}, ±φ<sup>3</sup>{{radic|8}}, ±φ<sup>3</sup>{{radic|8}}) relative to origin at the cell center. They form a cube (dashed lines) of edge length {{sfrac|1|φ{{radic|2}}}} ≈ 0.437 (the pentagon diagonal, and the '''#2 chord''' of the 120-cell). The face diagonals of the cube (not shown) of edge length {{sfrac|1|φ}} ≈ 0.618 are the edges of tetrahedral cells inscribed in the cube (600-cell edges, and the '''#3 chord''' of the 120-cell). The diameter of the dodecahedron is {{sfrac|{{radic|3}}|φ{{radic|2}}}} ≈ 0.757 (the cube diagonal, and the '''#4 chord''' of the 120-cell).|name=dodecahedral cell metrics}}]]

Reciprocally, the unit-radius 120-cell can be constructed just outside a 600-cell of slightly smaller long radius {{sfrac|φ<sup>2</sup>|{{radic|8}}}} ≈ 0.926, by placing the center of each dodecahedral cell at one of the 120 600-cell vertices. The 120-cell whose coordinates are given [[#√8 radius coordinates|above]] of long radius {{Radic|8}} = 2{{Radic|2}} ≈ 2.828 and edge-length {{sfrac|2|φ<sup>2</sup>}} = 3−{{radic|5}} ≈ 0.764 can be constructed in this manner just outside a 600-cell of long radius φ<sup>2</sup>, which is smaller than {{Radic|8}} in the same ratio of ≈ 0.926; it is in the golden ratio to the edge length of the 600-cell, so that must be φ. The 120-cell of edge-length 2 and long radius φ<sup>2</sup>{{Radic|8}} ≈ 7.405 given by Coxeter{{Sfn|Coxeter|1973|loc=Table I(ii); "120-cell"|pp=292-293}} can be constructed in this manner just outside a 600-cell of long radius φ<sup>4</sup> and edge-length φ<sup>3</sup>.

Therefore, the unit-radius 120-cell can be constructed from its predecessor the unit-radius 600-cell in three reciprocation steps.

==== Cell rotations of inscribed duals ====
Since the 120-cell contains inscribed 600-cells, it contains its own dual of the same radius. The 120-cell contains five disjoint 600-cells (ten overlapping inscribed 600-cells of which we can pick out five disjoint 600-cells in two different ways), so it can be seen as a compound of five of its own dual (in two ways). The vertices of each inscribed 600-cell are vertices of the 120-cell, and (dually) each dodecahedral cell center is a tetrahedral cell center in each of the inscribed 600-cells. 

The dodecahedral cells of the 120-cell have tetrahedral cells of the 600-cells inscribed in them.{{Sfn|Sullivan|1991|loc=The Dodecahedron|pp=4-5}} Just as the 120-cell is a compound of five 600-cells (in two ways), the dodecahedron is a compound of five regular tetrahedra (in two ways). As two opposing tetrahedra can be inscribed in a cube, and five cubes can be inscribed in a dodecahedron, ten tetrahedra in five cubes can be inscribed in a dodecahedron: two opposing sets of five, with each set covering all 20 vertices and each vertex in two tetrahedra (one from each set, but not the opposing pair of a cube obviously).{{Sfn|Coxeter|du Val|Flather|Petrie|1938|p=4|ps=; "Just as a tetrahedron can be inscribed in a cube, so a cube can be inscribed in a dodecahedron. By reciprocation, this leads to an octahedron circumscribed about an icosahedron. In fact, each of the twelve vertices of the icosahedron divides an edge of the octahedron according to the "[[golden section]]". Given the icosahedron, the circumscribed octahedron can be chosen in five ways, giving a [[compound of five octahedra]], which comes under our definition of [[stellated icosahedron]]. (The reciprocal compound, of five cubes whose vertices belong to a dodecahedron, is a stellated [[triacontahedron]].) Another stellated icosahedron can at once be deduced, by stellating each octahedron into a [[stella octangula]], thus forming a [[compound of ten tetrahedra]]. Further, we can choose one tetrahedron from each stella octangula, so as to derive a [[compound of five tetrahedra]], which still has all the rotation symmetry of the icosahedron (i.e. the icosahedral group), although it has lost the reflections. By reflecting this figure in any plane of symmetry of the icosahedron, we obtain the complementary set of five tetrahedra. These two sets of five tetrahedra are enantiomorphous, i.e. not directly congruent, but related like a pair of shoes. [Such] a figure which possesses no plane of symmetry (so that it is enantiomorphous to its mirror-image) is said to be ''[[chiral]]''."}} This shows that the 120-cell contains, among its many interior features, 120 [[Compound of ten tetrahedra|compounds of ten tetrahedra]], each of which is dimensionally analogous to the whole 120-cell as a compound of ten 600-cells.{{Efn|The 600 vertices of the 120-cell can be partitioned into those of 5 disjoint inscribed 120-vertex 600-cells in two different ways.{{Sfn|Waegell|Aravind|2014|pp=5-6}} The geometry of this 4D partitioning is dimensionally analogous to the 3D partitioning of the 20 vertices of the dodecahedron into 5 disjoint inscribed tetrahedra, which can also be done in two different ways because [[#Cell rotations of inscribed duals|each dodecahedral cell contains two opposing sets of 5 disjoint inscribed tetrahedral cells]]. The 120-cell can be partitioned in a manner analogous to the dodecahedron because each of its dodecahedral cells contains one tetrahedral cell from each of the 10 inscribed 600-cells.|name=2 ways to get 5 disjoint 600-cells}}

All ten tetrahedra can be generated by two chiral five-click rotations of any one tetrahedron. In each dodecahedral cell, one tetrahedral cell comes from each of the ten 600-cells inscribed in the 120-cell.{{Efn|The 10 tetrahedra in each dodecahedron overlap; but the 600 tetrahedra in each 600-cell do not, so each of the 10 must belong to a different 600-cell.}} Therefore the whole 120-cell, with all ten inscribed 600-cells, can be generated from just one 600-cell by rotating its cells.

==== Augmentation ====
Another consequence of the 120-cell containing inscribed 600-cells is that it is possible to construct it by placing [[Hyperpyramid|4-pyramid]]s of some kind on the cells of the 600-cell. These tetrahedral pyramids must be quite irregular in this case (with the apex blunted into four 'apexes'), but we can discern their shape in the way a tetrahedron lies inscribed in a [[Regular dodecahedron#Cartesian coordinates|dodecahedron]].{{Efn|name=truncated apex}}

Only 120 tetrahedral cells of each 600-cell can be inscribed in the 120-cell's dodecahedra; its other 480 tetrahedra span dodecahedral cells. Each dodecahedron-inscribed tetrahedron is the center cell of a [[600-cell#Icosahedra|cluster of five tetrahedra]], with the four others face-bonded around it lying only partially within the dodecahedron. The central tetrahedron is edge-bonded to an additional 12 tetrahedral cells, also lying only partially within the dodecahedron.{{Efn|As we saw in the [[600-cell#Cell clusters|600-cell]], these 12 tetrahedra belong (in pairs) to the 6 [[600-cell#Icosahedra|icosahedral clusters]] of twenty tetrahedral cells which surround each cluster of five tetrahedral cells.}} The central cell is vertex-bonded to 40 other tetrahedral cells which lie entirely outside the dodecahedron.

==== Weyl orbits ====
Another construction method uses [[quaternions]] and the [[Icosahedral symmetry]] of [[Weyl group]] orbits <math>O(\Lambda)=W(H_4)=I</math> of order 120.{{Sfn|Koca|Al-Ajmi|Ozdes Koca|2011|loc=6. Dual of the snub 24-cell|pp=986-988}} The following describe <math>T</math> and <math>T'</math> [[24-cell]]s as quaternion orbit weights of D4 under the Weyl group W(D4):<br/>
O(0100) : T = {±1,±e1,±e2,±e3,(±1±e1±e2±e3)/2}<br/>
O(1000) : V1<br/>
O(0010) : V2<br/>
O(0001) : V3

<math display="block">T'=\sqrt{2}\{V1\oplus V2\oplus V3 \} = \begin{pmatrix}
\frac{-1-e_1}{\sqrt{2}} & \frac{1-e_1}{\sqrt{2}} &
\frac{-1+e_1}{\sqrt{2}} & \frac{1+e_1}{\sqrt{2}} &
\frac{-e_2-e_3}{\sqrt{2}} & \frac{e_2-e_3}{\sqrt{2}} &
\frac{-e_2+e_3}{\sqrt{2}} & \frac{e_2+e_3}{\sqrt{2}}
\\
\frac{-1-e_2}{\sqrt{2}} & \frac{1-e_2}{\sqrt{2}} &
\frac{-1+e_2}{\sqrt{2}} & \frac{1+e_2}{\sqrt{2}} &
\frac{-e_1-e_3}{\sqrt{2}} & \frac{e_1-e_3}{\sqrt{2}} &
\frac{-e_1+e_3}{\sqrt{2}} & \frac{e_1+e_3}{\sqrt{2}}
\\
\frac{-e_1-e_2}{\sqrt{2}} & \frac{e_1-e_2}{\sqrt{2}} &
\frac{-e_1+e_2}{\sqrt{2}} & \frac{e_1+e_2}{\sqrt{2}} &
\frac{-1-e_3}{\sqrt{2}} & \frac{1-e_3}{\sqrt{2}} &
\frac{-1+e_3}{\sqrt{2}} & \frac{1+e_3}{\sqrt{2}}
\end{pmatrix};</math>

With quaternions <math>(p,q)</math> where <math>\bar p</math> is the conjugate of <math>p</math> and <math>[p,q]:r\rightarrow r'=prq</math> and <math>[p,q]^*:r\rightarrow r''=p\bar rq</math>, then the [[Coxeter group]] <math>W(H_4)=\lbrace[p,\bar p] \oplus [p,\bar p]^*\rbrace </math> is the symmetry group of the [[600-cell]] and the 120-cell of order 14400.

Given <math>p \in T</math> such that <math>\bar p=\pm p^4, \bar p^2=\pm p^3, \bar p^3=\pm p^2, \bar p^4=\pm p</math> and <math>p^\dagger</math> as an exchange of <math>-1/\varphi \leftrightarrow \varphi</math> within <math>p</math>, we can construct:

* the [[snub 24-cell]] <math>S=\sum_{i=1}^4\oplus p^i T</math>
* the [[600-cell]] <math>I=T+S=\sum_{i=0}^4\oplus p^i T</math> 
* the 120-cell <math>J=\sum_{i,j=0}^4\oplus p^i\bar p^{\dagger j}T'</math>
* the alternate snub 24-cell <math>S'=\sum_{i=1}^4\oplus p^i\bar p^{\dagger i}T'</math>
* the [[dual snub 24-cell]] = <math>T \oplus T' \oplus S'</math>.

=== As a configuration ===
This [[Regular 4-polytope#As configurations|configuration matrix]] represents the 120-cell. The rows and columns correspond to vertices, edges, faces, and cells. The diagonal numbers say how many of each element occur in the whole 120-cell. The nondiagonal numbers say how many of the column's element occur in or at the row's element.{{Sfn|Coxeter|1973|loc=§1.8 Configurations}}{{Sfn|Coxeter|1991|p=117}}

<math>\begin{bmatrix}\begin{matrix}600 & 4 & 6 & 4 \\ 2 & 1200 & 3 & 3 \\ 5 & 5 & 720 & 2 \\ 20 & 30 & 12 & 120 \end{matrix}\end{bmatrix}</math>

Here is the configuration expanded with ''k''-face elements and ''k''-figures. The diagonal element counts are the ratio of the full [[Coxeter group]] order, 14400, divided by the order of the subgroup with mirror removal.
{| class=wikitable
!H<sub>4</sub>||{{CDD|node_1|5|node|3|node|3|node}}
! [[k-face|''k''-face]]||f<sub>k</sub>||f<sub>0</sub> || f<sub>1</sub>||f<sub>2</sub>||f<sub>3</sub>||[[vertex figure|''k''-fig]]
!Notes
|- align=right
|A<sub>3</sub> || {{CDD|node_x|2|node|3|node|3|node}} ||( ) 
!f<sub>0</sub>
|| 600 || 4 || 6 || 4 ||[[regular tetrahedron|{3,3}]] || H<sub>4</sub>/A<sub>3</sub> = 14400/24 = 600
|- align=right
|A<sub>1</sub>A<sub>2</sub> ||{{CDD|node_1|2|node_x|2|node|3|node}} ||{ }
!f<sub>1</sub>
||   2 || 1200 ||    3 ||   3 || [[equilateral triangle|{3}]] || H<sub>4</sub>/A<sub>2</sub>A<sub>1</sub> = 14400/6/2 = 1200
|- align=right
|H<sub>2</sub>A<sub>1</sub> ||{{CDD|node_1|5|node|2|node_x|2|node}} ||[[pentagon|{5}]]
!f<sub>2</sub>
||   5 ||   5 || 720 ||   2 || { } || H<sub>4</sub>/H<sub>2</sub>A<sub>1</sub> = 14400/10/2 = 720
|- align=right
|H<sub>3</sub> ||{{CDD|node_1|5|node|3|node|2|node_x}} ||[[regular dodecahedron|{5,3}]]
!f<sub>3</sub>
||  20 || 30 || 12 ||120|| ( ) || H<sub>4</sub>/H<sub>3</sub> = 14400/120 = 120
|}

== Visualization ==
The 120-cell consists of 120 dodecahedral cells.  For visualization purposes, it is convenient that the dodecahedron has opposing parallel faces (a trait it shares with the cells of the [[tesseract]] and the [[24-cell]]).  One can stack dodecahedrons face to face in a straight line bent in the 4th direction into a great circle with a circumference of 10 cells.  Starting from this initial ten cell construct there are two common visualizations one can use: a layered stereographic projection, and a structure of intertwining rings.{{Sfn|Sullivan|1991|p=15|loc=Other Properties of the 120-cell}}

=== Layered stereographic projection ===
The cell locations lend themselves to a hyperspherical description.{{Sfn|Schleimer|Segerman|2013|p=16|loc=§6.1. Layers of dodecahedra}}  Pick an arbitrary dodecahedron and label it the "north pole".  Twelve great circle meridians (four cells long) radiate out in 3 dimensions, converging at the fifth "south pole" cell.  This skeleton accounts for 50 of the 120 cells (2 + 4 × 12).

Starting at the North Pole, we can build up the 120-cell in 9 latitudinal layers, with allusions to terrestrial 2-sphere topography in the table below.  With the exception of the poles, the centroids of the cells of each layer lie on a separate 2-sphere, with the equatorial centroids lying on a great 2-sphere. The centroids of the 30 equatorial cells form the vertices of an [[icosidodecahedron]], with the meridians (as described above) passing through the center of each pentagonal face. The cells labeled "interstitial" in the following table do not fall on meridian great circles.

{| class="wikitable"
|-
! Layer #
! Number of Cells
! Description
! Colatitude
! Region
|-
| style="text-align: center" | 1
| style="text-align: center" | 1 cell
| North Pole
| style="text-align: center" | 0°
| rowspan="4" | Northern Hemisphere
|-
| style="text-align: center" | 2
| style="text-align: center" | 12 cells
| First layer of meridional cells / "[[Arctic Circle]]"
| style="text-align: center" | 36°
|-
| style="text-align: center" | 3
| style="text-align: center" | 20 cells
| Non-meridian / interstitial
| style="text-align: center" | 60°
|-
| style="text-align: center" | 4
| style="text-align: center" | 12 cells
| Second layer of meridional cells / "[[Tropic of Cancer]]"
| style="text-align: center" | 72°
|-
| style="text-align: center" | 5
| style="text-align: center" | 30 cells
| Non-meridian / interstitial
| style="text-align: center" | 90°
| style="text-align: center" | Equator
|-
| style="text-align: center" | 6
| style="text-align: center" | 12 cells
| Third layer of meridional cells / "[[Tropic of Capricorn]]"
| style="text-align: center" | 108°
| rowspan="4" | Southern Hemisphere
|-
| style="text-align: center" | 7
| style="text-align: center" | 20 cells
| Non-meridian / interstitial
| style="text-align: center" | 120°
|-
| style="text-align: center" | 8
| style="text-align: center" | 12 cells
| Fourth layer of meridional cells / "[[Antarctic Circle]]"
| style="text-align: center" | 144°
|-
| style="text-align: center" | 9
| style="text-align: center" | 1 cell
| South Pole
| style="text-align: center" | 180°
|-
! Total
! 120 cells
! colspan="3" |
|}
The cells of layers 2, 4, 6 and 8 are located over the faces of the pole cell. The cells of layers 3 and 7 are located directly over the vertices of the pole cell.  The cells of layer 5 are located over the edges of the pole cell.

=== Intertwining rings ===
[[Image:120-cell rings.jpg|right|thumb|300px|Two intertwining rings of the 120-cell.]]
[[File:120-cell_two_orthogonal_rings.png|thumb|300px|Two orthogonal rings in a cell-centered projection]]
The 120-cell can be partitioned into 12 disjoint 10-cell great circle rings, forming a discrete/quantized [[Hopf fibration]].{{Sfn|Coxeter|1970|loc=§9. The 120-cell and the 600-cell|pp=19-23}}{{Sfn|Schleimer|Segerman|2013|pp=16-18|loc=§6.2. Rings of dodecahedra}}{{Sfn|Banchoff|2013}}{{Sfn|Zamboj|2021|pp=6-12|loc=§2 Mathematical background}}{{Sfn|Sullivan|1991|loc=Other Properties of the 120-cell|p=15}} Starting with one 10-cell ring, one can place another ring alongside it that spirals around the original ring one complete revolution in ten cells.  Five such 10-cell rings can be placed adjacent to the original 10-cell ring.  Although the outer rings "spiral" around the inner ring (and each other), they actually have no helical [[Torsion of a curve|torsion]].  They are all equivalent.  The spiraling is a result of the 3-sphere curvature.  The inner ring and the five outer rings now form a six ring, 60-cell solid torus. One can continue adding 10-cell rings adjacent to the previous ones, but it's more instructive to construct a second torus, disjoint from the one above, from the remaining 60 cells, that interlocks with the first.  The 120-cell, like the 3-sphere, is the union of these two ([[Clifford torus|Clifford]]) tori.  If the center ring of the first torus is a meridian great circle as defined above, the center ring of the second torus is the equatorial great circle that is centered on the meridian circle.{{Sfn|Zamboj|2021|loc=§5 Hopf tori corresponding to circles on B<sup>2</sup>|pp=23-29}} Also note that the spiraling shell of 50 cells around a center ring can be either left handed or right handed.  It's just a matter of partitioning the cells in the shell differently, i.e. picking another set of disjoint ([[Clifford parallel]]) great circles.

=== Other great circle constructs ===
There is another great circle path of interest that alternately passes through opposing cell vertices, then along an edge.  This path consists of 6 edges alternating with 6 cell diameter [[#Chords|chords]], forming an irregular dodecagon in a central plane.{{Efn|[[File:Great dodecagon of the 120-cell.png|thumb|200px|The 120-cell has 200 central planes that each intersect 12 vertices, forming an irregular dodecagon with alternating edges of two different lengths. Inscribed in the dodecagon are two regular great hexagons (black),{{Efn|name=great hexagon}} two irregular great hexagons ({{Color|red|red}}),{{Efn|name=irregular great hexagon}} and four equilateral great triangles (only one is shown, in {{Color|green|green}}).]]The 120-cell has an irregular [[#Other great circle constructs|dodecagon {12} great circle polygon]] of 6 edges (#1 [[#Chords|chords]] marked {{Color|red|𝜁}}) alternating with 6 dodecahedron cell-diameters ({{Color|magenta|#4}} chords).{{Efn|name=dodecahedral cell metrics}} The irregular great dodecagon contains two irregular great hexagons ({{color|red|red}}) inscribed in alternate positions.{{Efn|name=irregular great hexagon}} Two ''regular'' great hexagons with edges of a third size ({{radic|1}}, the #5 chord) are also inscribed in the dodecagon.{{Efn|name=great hexagon}} The twelve regular hexagon edges (#5 chords), the six cell-diameter edges of the dodecagon (#4 chords), and the six 120-cell edges of the dodecagon (#1 chords), are all chords of the same great circle, but the other 24 zig-zag edges (#1 chords, not shown) that bridge the six #4 edges of the dodecagon do not lie in this great circle plane. The 120-cell's irregular great dodecagon planes, its irregular great hexagon planes, its regular great hexagon planes, and its equilateral great triangle planes, are the same set of dodecagon planes. The 120-cell contains 200 such {12} central planes (100 completely orthogonal pairs), the ''same'' 200 central planes each containing a [[600-cell#Hexagons|hexagon]] that are found in each of the 10 inscribed 600-cells.{{Efn|The 120-cell contains ten 600-cells which can be partitioned into five completely disjoint 600-cells two different ways.{{Efn|name=2 ways to get 5 disjoint 600-cells}} All ten 600-cells occupy the same set of 200 irregular great dodecagon central planes.{{Efn|name=irregular great dodecagon}} There are exactly 400 regular hexagons in the 120-cell (two in each dodecagon central plane), and each of the ten 600-cells contains its own distinct subset of 200 of them (one from each dodecagon central plane). Each 600-cell contains only one of the two opposing regular hexagons inscribed in any dodecagon central plane, just as it contains only one of two opposing tetrahedra inscribed in any dodecahedral cell. Each 600-cell is disjoint from 4 other 600-cells, and shares hexagons with 5 other 600-cells.{{Efn|Each regular great hexagon is shared by two 24-cells in the same 600-cell,{{Efn|1=A 24-cell contains 16 hexagons. In the 600-cell, with 25 24-cells, each 24-cell is disjoint from 8 24-cells and intersects each of the other 16 24-cells in six vertices that form a hexagon.{{Sfn|Denney|Hooker|Johnson|Robinson|2020|p=438}} A 600-cell contains 25・16/2 = 200 such hexagons.|name=disjoint from 8 and intersects 16}} and each 24-cell is shared by two 600-cells.{{Efn|name=two 600-cells share a 24-cell}} Each regular hexagon is shared by four 600-cells.|name=hexagons 24-cells and 600-cells}} Each disjoint pair of 600-cells occupies the opposing pair of disjoint great hexagons in every dodecagon central plane. Each non-disjoint pair of 600-cells intersects in 16 hexagons that comprise a 24-cell. The 120-cell contains 9 times as many distinct 24-cells (225) as disjoint 24-cells (25).{{Efn|name=rays and bases}} Each 24-cell occurs in 9 600-cells, is absent from just one 600-cell, and is shared by two 600-cells.|name=same 200 planes}}|name=irregular great dodecagon}}  Both these great circle paths have dual [[600-cell#Union of two tori|great circle paths in the 600-cell]].  The 10 cell face to face path above maps to a 10 vertex path solely traversing along edges in the 600-cell, forming a [[600-cell#Decagons|decagon]].{{Efn|name=two coaxial Petrie 30-gons}} The alternating cell/edge path maps to a path consisting of 12 tetrahedrons alternately meeting face to face then vertex to vertex (six [[triangular bipyramids]]) in the 600-cell.  This latter path corresponds to a [[600-cell#Icosahedra|ring of six icosahedra]] meeting face to face in the [[snub 24-cell]] (or [[icosahedral pyramids]] in the 600-cell).

Another great circle polygon path exists which is unique to the 120-cell and has no dual counterpart in the 600-cell. This path consists of 3 120-cell edges alternating with 3 inscribed 5-cell edges (#8 chords), forming the irregular great hexagon with alternating short and long edges [[120-cell#Chords|illustrated above]].{{Efn|name=irregular great hexagon}} Each 5-cell edge runs through the volume of three dodecahedral cells (in a ring of ten face-bonded dodecahedral cells), to the opposite pentagonal face of the third dodecahedron. This irregular great hexagon lies in the same central plane (on the same great circle) as the irregular great dodecagon described above, but it intersects only {6} of the {12} dodecagon vertices. There are two irregular great hexagons inscribed in each irregular great dodecagon, in alternate positions.{{Efn|name=irregular great dodecagon}}

=== Perspective projections ===
{|class="wikitable"
!colspan=2|Projections to 3D of a 4D 120-cell performing a [[SO(4)#Geometry of 4D rotations|simple rotation]]
|-
|align=center|[[File:120-cell.gif|256px]]
|align=center|[[File:120-cell-inner.gif|256px]]
|-
|From outside the [[3-sphere]] in 4-space.
|Inside the [[600-cell#Boundary envelopes|3D surface]] of the 3-sphere.
|}

As in all the illustrations in this article, only the edges of the 120-cell appear in these renderings. All the other [[#Chords|chords]] are not shown. The complex [[#Relationships among interior polytopes|interior parts]] of the 120-cell, all its inscribed 600-cells, 24-cells, 8-cells, 16-cells and 5-cells, are completely invisible in all illustrations. The viewer must imagine them.

These projections use [[perspective projection]], from a specific viewpoint in four dimensions, projecting the model as a 3D shadow. Therefore, faces and cells that look larger are merely closer to the 4D viewpoint.

A comparison of perspective projections of the 3D dodecahedron to 2D (below left), and projections of the 4D 120-cell to 3D (below right), demonstrates two related perspective projection methods, by dimensional analogy. [[Schlegel diagram]]s use [[Perspective (graphical)|perspective]] to show depth in the dimension which has been flattened, choosing a view point ''above'' a specific cell, thus making that cell the envelope of the model, with other cells appearing smaller inside it. [[Stereographic projection]]s use the same approach, but are shown with curved edges, representing the spherical polytope as a tiling of a [[3-sphere]]. Both these methods distort the object, because the cells are not actually nested inside each other (they meet face-to-face), and they are all the same size. Other perspective projection methods exist, such as the rotating animations above, which do not exhibit this particular kind of distortion, but rather some other kind of distortion (as all projections must).

{| class="wikitable" style="width:540px;"
|+Comparison with regular dodecahedron
|-
!width=80|Projection
![[Dodecahedron]]
!120-cell
|-
![[Schlegel diagram]]
|align=center|[[Image:Dodecahedron schlegel.svg|220px]]<br>12 pentagon faces in the plane
|align=center|[[File:Schlegel wireframe 120-cell.png|220px]]<br>120 dodecahedral cells in 3-space
|-
![[Stereographic projection]]
|align=center|[[Image:Dodecahedron stereographic projection.png|220px]]
|align=center|[[Image:Stereographic polytope 120cell faces.png|220px]]<br>With transparent faces
|}

{|class="wikitable"
|-
!colspan=2|Enhanced perspective projections
|-
|align=center|[[Image:120-cell perspective-cell-first-02.png|240px]]
|Cell-first perspective projection at 5 times the distance from the center to a vertex, with these enhancements applied:
* Nearest dodecahedron to the 4D viewpoint rendered in yellow
* The 12 dodecahedra immediately adjoining it rendered in cyan;
* The remaining dodecahedra rendered in green;
* Cells facing away from the 4D viewpoint (those lying on the "far side" of the 120-cell) culled to minimize clutter in the final image.
|-
|align=center|[[Image:120-cell perspective-vertex-first-02.png|240px]]
|Vertex-first perspective projection at 5 times the distance from center to a vertex, with these enhancements:
* Four cells surrounding nearest vertex shown in 4 colors
* Nearest vertex shown in white (center of image where 4 cells meet)
* Remaining cells shown in transparent green
* Cells facing away from 4D viewpoint culled for clarity
|}

=== Orthogonal projections ===
[[Orthogonal projection]]s of the 120-cell can be done in 2D by defining two orthonormal basis vectors for a specific view direction. The 30-gonal projection was made in 1963 by [[B. L. Chilton]].{{Sfn|Chilton|1964}}

The H3 [[decagon]]al projection shows the plane of the [[van Oss polygon]].

{| class="wikitable"
|+ [[Orthographic projection]]s by [[Coxeter plane]]s{{Sfn|Dechant|2021|pp=18-20|loc=6. The Coxeter Plane}}
|- align=center
!H<sub>4</sub>
! -
!F<sub>4</sub>
|- align=center
|[[File:120-cell graph H4.svg|240px]]<br>[30]<br>(Red=1)
|[[File:120-cell t0 p20.svg|240px]]<br>[20]<br>(Red=1)
|[[File:120-cell t0 F4.svg|240px]]<br>[12]<br>(Red=1)
|- align=center
!H<sub>3</sub>
!A<sub>2</sub> / B<sub>3</sub> / D<sub>4</sub>
!A<sub>3</sub> / B<sub>2</sub>
|- align=center
|[[File:120-cell t0 H3.svg|240px]]<br>[10]<br>(Red=5, orange=10)
|[[File:120-cell t0 A2.svg|240px]]<br>[6]<br>(Red=1, orange=3, yellow=6, lime=9, green=12)
|[[File:120-cell t0 A3.svg|240px]]<br>[4]<br>(Red=1, orange=2, yellow=4, lime=6, green=8)
|}

3-dimensional orthogonal projections can also be made with three orthonormal basis vectors, and displayed as a 3d model, and then projecting a certain perspective in 3D for a 2d image.

{| class="wikitable" style="width:540px;"
|+3D orthographic projections
|[[File:120Cell 3D.png|270px]]<br>3D isometric projection
|align=center|[[File:Cell120.ogv|270px]]<br>Animated 4D rotation
|}

== Related polyhedra and honeycombs==

=== H<sub>4</sub> polytopes ===
The 120-cell is one of 15 regular and uniform polytopes with the same H<sub>4</sub> symmetry [3,3,5]:{{Sfn|Denney|Hooker|Johnson|Robinson|2020}}
{{H4_family}}

=== {p,3,3} polytopes ===
The 120-cell is similar to three [[regular 4-polytopes]]: the [[5-cell]] {3,3,3} and [[tesseract]] {4,3,3} of Euclidean 4-space, and the [[hexagonal tiling honeycomb]] {6,3,3} of hyperbolic space. All of these have a [[tetrahedral]] [[vertex figure]] {3,3}:
{{Tetrahedral vertex figure tessellations small}}

=== {5,3,p} polytopes ===
The 120-cell is a part of a sequence of 4-polytopes and honeycombs with [[dodecahedral]] cells:
{{Dodecahedral_tessellations_small}}

=== Tetrahedrally diminished 120-cell ===
Since the 600-point 120-cell has 5 disjoint inscribed 600-cells, it can be diminished by the removal of one of those 120-point 600-cells, creating an irregular 480-point 4-polytope.{{Efn|The diminishment of the 600-point 120-cell to a 480-point 4-polytope by removal of one if its 600-cells is analogous to the [[600-cell#Diminished 600-cells|diminishment of the 120-point 600-cell]] by removal of one of its 5 disjoint inscribed 24-cells, creating the 96-point [[snub 24-cell]]. Similarly, the 8-cell tesseract can be seen as a 16-point [[24-cell#Diminishings|diminished 24-cell]] from which one 8-point 16-cell has been removed.}} 

[[File:Tetrahedrally_diminished_regular_dodecahedron.png|thumb|In the [[tetrahedrally diminished dodecahedron]], 4 vertices are truncated to equilateral triangles. The 12 pentagon faces lose a vertex, becoming trapezoids.]]
Each dodecahedral cell of the 120-cell is diminished by removal of 4 of its 20 vertices, creating an irregular 16-point polyhedron called the [[tetrahedrally diminished dodecahedron]] because the 4 vertices removed formed a [[#Dual 600-cells|tetrahedron inscribed in the dodecahedron]]. Since the vertex figure of the dodecahedron is the triangle, each truncated vertex is replaced by a triangle. The 12 pentagon faces are replaced by 12 trapezoids, as one vertex of each pentagon is removed and two of its edges are replaced by the pentagon's diagonal chord.{{Efn|name=face pentagon chord}} The tetrahedrally diminished dodecahedron has 16 vertices and 16 faces: 12 trapezoid faces and four equilateral triangle faces. 

Since the vertex figure of the 120-cell is the tetrahedron,{{Efn|Each 120-cell vertex figure is actually a low tetrahedral pyramid, an irregular [[5-cell]] with a regular tetrahedron base.|name=truncated apex}} each truncated vertex is replaced by a tetrahedron, leaving 120 tetrahedrally diminished dodecahedron cells and 120 regular tetrahedron cells. The regular dodecahedron and the tetrahedrally diminished dodecahedron both have 30 edges, and the regular 120-cell and the tetrahedrally diminished 120-cell both have 1200 edges.

The '''480-point diminished 120-cell''' may be called the '''tetrahedrally diminished 120-cell''' because its cells are tetrahedrally diminished, or the '''600-cell diminished 120-cell''' because the vertices removed formed a 600-cell inscribed in the 120-cell, or even the '''regular 5-cells diminished 120-cell''' because removing the 120 vertices removes one vertex from each of the 120 inscribed regular 5-cells, leaving 120 regular tetrahedra.{{Efn|name=inscribed 5-cells}}

=== Davis 120-cell ===
The '''Davis 120-cell''', introduced by {{harvtxt|Davis|1985}}, is a compact 4-dimensional [[hyperbolic manifold]] obtained by identifying opposite faces of the 120-cell, whose universal cover gives the [[List of regular polytopes#Tessellations of hyperbolic 4-space|regular honeycomb]] [[order-5 120-cell honeycomb|{5,3,3,5}]] of 4-dimensional hyperbolic space.

==See also==
*[[Uniform 4-polytope#The H4 family|Uniform 4-polytope family with [5,3,3] symmetry]]
*[[57-cell]] – an abstract regular [[4-polytope]] constructed from 57 hemi-dodecahedra.
*[[600-cell]] - the dual [[4-polytope]] to the 120-cell

==Notes==
{{Notelist}}

==Citations==
{{Reflist}}

==References==
{{Refbegin}}
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{{Refend}}

==External links==
* {{MathWorld | urlname = 120-Cell | title = 120-Cell}}
*{{GlossaryForHyperspace | anchor=hecatonicosachoron | title=Hecatonicosachoron}}
** {{PolyCell | urlname = section4.html| title = Convex uniform polychora based on the hecatonicosachoron (120-cell) and hexacosichoron (600-cell) - Model 32}}
* {{KlitzingPolytopes|polychora.htm|4D uniform polytopes (polychora)|o3o3o5x - hi}}
* [http://www.polytope.de/c120.html Der 120-Zeller (120-cell)] Marco Möller's Regular polytopes in R<sup>4</sup> (German)
*[http://www.gravitation3d.com/120cell/ 120-cell explorer] &ndash; A free interactive program that allows you to learn about a number of the 120-cell symmetries.  The 120-cell is projected to 3 dimensions and then rendered using OpenGL.
* [http://www.theory.org/geotopo/120-cell/ Construction of the Hyper-Dodecahedron]
* [https://www.youtube.com/watch?v=MFXRRW9goTs/ YouTube animation of the construction of the 120-cell]  Gian Marco Todesco.

{{H4_family}}
{{Regular 4-polytopes}}
{{Polytopes}}
{{Authority control}}

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