First, let's have a look around!

Fig. 1a: A wide view of the office. Photo by Aris Noutsos.

Fig. 1b: A narrower view towards some of the most complex models of 4-dimensional polytopes.
Photo by Aris Noutsos.

Fig. 1c:
This is me in my polytope garden, holding a projection of the Grand Antiprism in 3 dimensions! Photo by Aris Noutsos.

Polyhedra, and more generally polytopes are, among mathematical concepts, one of the easiest to understand and visualize. This makes them a gateway to that higher world of order and beauty which lies beyond our own.

This special feature of polyhedra is what motivated me to build these models. In the late 1990's - early 2000's I built a significant number of models of Uniform polyhedra; these are in my parents' country house, in Portugal. The recent models, built since 2009 and currently in my office, are the topic of this page; these include (since 2014) 3-D shadows of the 4-dimensional analogues of polyhedra, the polychora.

News:

2019 January 26: built model of Gosset's 8-dimensional figure. This was later disassembled.

2018 December 19: completed the compound of 15 16-cells.

2018 August 4: Completed the compound of 5 24-cells.

2017 November 11: Completed the Great grand stellated 120-cell. This completes the list of projections of all 16 regular polychora.

2017 November 2: Some of my models are being displayed at the Gutenberg store in Bad Godesberg. See poster here by Ⓒ Zometool Europa / Lyn Taylor, with photos by Aris Noutsos and Jason Wu.

2016 November 12: Completed larger scale version of the rectified 120-cell. Later disassembled.

2016 February 13: Completed rectified 600-cell. Later disassembled.

2015: Moved to new office.

2014 August 21: Completed model of the Grand 600-cell.

2014 August 6: Completed model of the stellated 120-cell.

In ``King of Infinite Space: Donald Coxeter, the Man Who Saved Geometry'', by Siobhan Roberts.

From 2009 to 2013, I built a small collection of geometric paper models for my office, which includes a few of the uniform polyhedra and their duals:

- The nine regular polyhedra. These are transitive on their vertices (isogonal), on their edges (isotoxal) and faces (isohedral). It follows from this that their faces are regular polygons, i.e., the faces are regular.
- The seven quasi-regular polyhedra. These are isogonal and isotoxal but not isohedral (the faces are all regular, but not all identical).
- The quasi-regular dual polyhedra. These are isotoxal and isohedral, but not isogonal (the faces are all identical, but not regular).

Different Wythoff constructions would result in other types of uniform polyhedra, like the remaining Archimedean polyhedra (which include the Truncated icosahedron that everyone asks about when they come to my office - no, I don't have that model in my office).

For the following pictures of polyhedra, the colour code is as follows: the non-regular faces are blue, they belong to the duals of the quasi-regular polyhedra; for the regular faces, the equilateral triangles are yellow, squares are red, pentagons are green and pentagrams are gold. Since the latter are regular polygons, the polyhedra built from them shown below are either regular or quasi-regular. Thus, when we discuss e.g., the regular Tetrahedron, we use simply the word Tetrahedron, and likewise for Octahedron, Icosahedron and Dodecahedron.

Fig. 2: The convex polyhedra. Bottom row, from right to left:
1 - The Tetrahedron
(the only model that has tetrahedral symmetry), 2 - its rectification,
the Octahedron, 3 - the
dual of the Octahedron,
the Cube,
4 - the rectification of the Cube and Octahedron - the Cuboctahedron and 5 - the dual of the Cuboctahedron,
the Rhombic dodecahedron
(these last four have octahedral symmetry).
Top row, right to left:
1 - the Icosahedron and 2 -
its dual, the Dodecahedron,
3 - the rectification of the Icosahedron and the Dodecahedron -
the Icosidodecahedron and
4 - the dual of the Icosidodecahedron,
the Rhombic triacontahedron
(these four have icosahedral symmetry).
The five polyhedra on the right (Tetrahedron, Octahedron, Cube, Icosahedron and Dodecahedron) are the
five platonic polyhedra, the
only regular convex polyhedra. The Cuboctahedron and Icosidodecahedron
(those with two colors) are the only convex quasi-regular polyhedra, and the
two rhombic polyhedra in blue are their duals.

Frame of picture taken by Jason Wu.

Fig. 3: The platonic polyhedra, this time as dice. Picture by Aris Noutsos.

A few notes on the non-convex polyhedra that follow:

- They all have icosahedral symmetry,
- The vertices of all regular and quasi-regular polyhedra, like all uniform polyhedra, belong to a sphere that circumscribes the whole polyhedron and is concentric with it. The inner vertices are false: several edges intersect there, but none ends there. In what follows, we generally refer only to the true vertices.
- These vertices are arranged as either the Dodecahedron, Icosahedron or Icosidodecahedron in Fig. 3, i.e., they are facetings of these convex polyhedra which are therefore their convex hulls. By a general rule, their dual polyhedra are stellations of the duals of their convex hulls (The reason for this is simple: take line from a vertex to the centre of a polyhedron. The face of the dual polyhedron is perpendicular to this line. Thus, if we keep the same vertex arrangement for another polyhedron, we must keep the same set of perpendicular planes for the faces of its dual).

Fig. 4: The four Kepler-Poinsot polyhedra:
the Small stellated dodecahedron (top left) and its dual,
the Great dodecahedron (bottom left),
the Great stellated dodecahedron (top right) and its dual, the
Great icosahedron (bottom right).

Frame of picture taken by Jason Wu.

The relations between the Dodecahedron, Icosahedron and the Kepler-Poinsot
polyhedra are displayed in Fig. 5 below. The vertical scale indicates the
density.
Duality is given by the two-sided golden arrows.
For each face of a polyhedron, there is a perpendicular line from the centre of the dual polyhedron to its vertex;
for each edge of a polyhedron, the dual polyhedron has a perpendicular edge. The duality operation
transforms the face of a polyhedron into the vertex figure of its dual.

There are two ``stellation'' operations, that extend the faces of a particular
polyhedron. The first, edge stellation, extends the edges of the faces (obviously
in the same direction, but both ways) until they meet again, this
is illustrated by the blue arrows. This can only start from polyhedra
with pentagonal faces. The second operation, Greatening,
replaces a face with a larger one of the same kind in
the same plane; this is displayed by the green arrows.
Both operations
conserve the number of faces and their planes; therefore all polyhedra derived from the
Dodecahedron (Great dodecahedron, Small stellated dodecahedron and Great dodecahedron) have
12 faces, as their names indicate. They represent the full set of
stellations of the Dodecahedron;
the model in Fig. 11b is useful to see how they can be derived
geometrically by the process of extending the planes of the faces.
The Great icosahedron, being a greatening of the Icosahedron, has 20 triangular faces.
It is the only of the 59 stellations the Icosahedron
that is regular.

In Fig. 5 we also present the faceting, or ``conservation'' operations, which as we describe
below are the duals of the stellation operations.
The solid red lines indicate faceting with conservation of
edge arrangement:
Indeed, the Great dodecahedron has the same edge arrangement as the Icosahedron,
and the Great icosahedron has the same edge arrangement of the Small stellated dodecahedron,
as can be seen in Fig. 4. The dashed lines in Fig. 5 indicate faceting with conservation of the
vertex figure.
Both the solid red lines and the dashed lines imply conservation of the vertex arrangement, which all faceting operations
must obey by definition.

It follows from these conservation laws that the four polyhedra in the red circuit must
share the same vertex arrangement - in this case of the Icosahedron. This means that
they are facetings of the Icosahedron (see point number 3 above when introducing the
non-convex polyhedra). The two polyhedra in the pink dotted line have the
vertex arrangement and vertex figure of the Dodecahedron.

Why these conservation relations exist is explained below.

Fig. 5: Relations between the Dodecahedron, Icosahedron and the Kepler-Poinsot polyhedra.

(Technical bit: please skip if you're devoid of curiosity).

Why do these conservation relations exist? The answer is because they can be described as
duals to the stellation operations. In particular:

1) Conservation of edges (red) = find dual + edge stellate + find dual

2) Conservation of vertex figure (dotted) = find dual + greaten + find dual

As an example of 1), let's move from the Icosahedron to the Great dodecahedron along the solid red line.
This is the same as finding the dual of the Icosahedron (Dodecahedron), edge stellating (Small stellated dodecahedron) and finding the dual of the latter
(Great dodecahedron). The first operation transformed the edges of the Icosahedron into the perpendicular edges, those
of the Dodecahedron. The second operation merely extended those edges, but kept their directions.
The last operation find edges perpendicular to those of the Small stellated dodecahedron - those of the original Icosahedron!

As an example of 2), let's move from the Dodecahedron to the Great stellated dodecahedron along the dotted pink line.
This is the same as finding the dual of the Dodecahedron (Icosahedron), greatening (Great Icosahedron) and finding the dual of the latter (Great
stellated dodecahedron).
The first duality converts the triangular vertex figure of the Dodecahedron into the triangular face of the Icosahedron.
Then greatening to a Great Icosahedron keeps the same type of face (as greatening always does).
In the final dual transformation, the triangular faces of the Great Icosahedron are converted back to triangular vertex figures, as in the original
Dodecahedron. Thus this operation preserves the vertex figure.

All faceting operations preserve the vertex arrangements. This is because their dual
(the stellation operations) preserve the planes of the faces.

(end of technical bit)

Fig. 6: Two quasi-regular star polyhedra and their duals. Top right:
the rectification of the Great dodecahedron and the Small stellated Icosahedron - the
Dodecadodecahedron, bottom right: its dual,
the Medial rhombic triacontahedron;
Top left:
the rectification of the Great Icosahedron and the Great stellated dodecahedron -
the Great icosidodecahedron, bottom left: its dual,
the Great rhombic triacontahedron.

The operation of rectification corresponds to finding the middle of the edges of a
polyhedron and transforming it in a new vertex. Doing this for any two dual polyhedra
results in the same polyhedron, since their edges are perpendicular and intersect at their midpoints.

Rectifying the Kepler-Poinsot polyhedra, we always obtain the vertex arrangement of the Icosidodecahedron.
We can see this easily from Fig. 5: the Small stellated dodecahedron can be obtained from the Dodecahedron
by a symmetric (both ways) edge stellation. Thus the arrangement of the mid-points of its edges remained unchanged
under edge stellation - it is still the arrangement of the vertices of the Icosidodecahedron.
The same necessarily applies to its dual, the Great dodecahedron.

The Great stellated dodecahedron can similarly be obtained from the Great dodecahedron by edge stellation,
therefore the mid-points of its edges still have the same arragement as the vertices of the Icosidodecahedron.
The same will necessarily apply to its dual, the Great icosahedron.

Thus these rectifications of the Kepler-Poinsot polyhedra (the
Dodecadodecahedron and the Great Icosidodecahedron in the top row) are facetings of the
Icosidodecahedron. This implies that their duals must be stellations of the dual of the Icosidodecahedron,
the Rhombic triacontahedron.

Frame of picture taken by Jason Wu.

Fig. 7: We now show a few of the facetings of the Dodecahedron, in particular
the ditrigonal
quasi-regular star polyhedra:
The Small ditrigonal icosidodecahedron (left) and its dual, the
Small triambic icosahedron
(centre left, in blue), the Ditrigonal dodecadodecahedron (centre right)
and its dual, the Medial triambic icosahedron (right, in blue),
the Great ditrigonal icosidodecahedron (far right, in the foreground)
and its dual, the Great triambic icosahedron (right, in blue) - this is represented by the same model as the Medial triambic icosahedron as they only differ in their internal structure.
Since the ditrigonal star polyhedra are facetings of the Dodecahedron, their duals
are, of course, stellations of the Icosahedron.

The three ditrigonal quasi-regular polyhedra all share the edge arrangement of the
compound of five cubes.
The edges of their duals (in blue) (and the dual of the compound of five cubes, the
compound of five octahedra) are perpendicular to the former, which means that they are all have the same directions - indeed, they can all be derived from the first stellation of the Icosahedron (the Small triambic icosahedron) by edge stellation.

Picture taken by Aris Noutsos.

Fig. 8a: Not all polyhedron models are made of paper. Here are stained glass models of the Icosidodecahedron (right) and of the Dodecadodecahedron (left). Made by Naomi Janches.

Fig. 8b: Here is a 3-D printed edge model of a
uniform polyhedron compound,
the compound of 20 Octahedra.

This set of edges is shared by two remarkable
uniform polyhedra. The first is the Great dirhombicosidodecahedron, a uniform polyhedron with a highly
unusual Wythoff construction.
For this reason it is also known as ``Miller's Monster".
This was the last entry in the 1954 list of uniform polyhedra compiled by J. C. P. Miller, H. S. M. Coxeter and M. S. Longuet-Higgins.

The other remarkable polyhedron that shares this set of edges is
the Great disnub dirhombidodecahedron.
The latter object was discovered in 1975 when John Skilling proved that
the 1954 list of uniform polyhedra is complete. In that paper he generalized the concept of Uniform polyhedron:
instead of two faces per edge, there can be any even number (or, equivalently, edges can be multiple).
This generalization adds only this new figure, for that reason this it is also known as ``Skilling's figure".

Finally, the edges also belong to another special uniform polyhedron compound, the Compound of twenty tetrahemihexahedra.

Model printed by Shapeways, design by
Mathematical Creations.

Before ending this section, it is important to remark that the regular and quasi-regular polyhedra shown above represent only a small fraction of the Uniform polyhedra. For more models of the latter, check Fig. 8b and my page on Uniform polyhedra.

H. S. M. Coxeter, in the preface to ``Regular Polytopes''.

In 2014 I started building Zometool models. Such models display only the edge arrangements of a geometrical object. Therefore, they cannot display face arrangements. A consequence of this is that the Icosahedron and the Great dodecahedron, which share the same edge arrangements, are represented by the same Zometool model. The same would happen for the Small stellated dodecahedron and the Great Icosahedron. The three ditrigonal quasi-regular polyhedra in Fig. 7 and the compound of five cubes are all represented by the same Zometool model (see below).

The main advantage of Zometool models, however, is that they allow the display of internal structure; for the models that follow that is absolutely necessary. As an example, in the Zometool model below I display a model that shows many geometric relations between the Platonic polyhedra. This particular kit also extremely useful for me to familiarize myself with the extremely interesting properties of Zometool, something that I suggest the reader does before attemptiong to build any of the models that follows.

Fig. 9: Myself holding a beautiful geometrical model that illustrates many interesting relations between the Platonic polyhedra and their
symmetries. This is sold by Zometool as Kepler's Kosmos,
and was designed originally by John H. Conway. Photo by Aris Noutsos.

The models below represent stellations of the five convex isohedral polyhedra shown in Fig. 3 that can be stellated. This set consists of 3 Platonic polyhedra (the Octahedron, Dodecahedron and Icosahedron) plus the Rhombic dodecahedron and Rhombic triacontahedron. Being isohedral, they have only one stellation diagram; this makes the model much easier to plan and results in more appealing models.

Among these stellations we find many of the polyhedra shown above plus some interesting regular polyhedron compounds.

Note: Three of these models use non-standard, extra-long Zometool parts. These can be built with regular parts with a ball and two struts, but the results are not so satisfying. If you'd like to acquire extra-long parts, I suggest purchasing old Zometool sets on eBay.

Fig. 10a: This is the stellation pattern of the Octahedron. The inner triangle is the face of the Octahedron.
The outer triangle is the face of its only stellation, known as the Stella Octangula.

Fig. 10b: Myself holding a model of the Stella Octangula.
Here we can see that this stellation can be seen as an intersection of two Tetrahedra. The outer vertices are those of a cube. Photo by Aris Noutsos.

Fig. 11a: This is the stellation pattern of the Dodecahedron; its face
is the inner pentagon. The inner pentagram is the face of the Small stellated dodecahedron.
The outer pentagon is the face of the Great Dodecahedron, and the outer pentagram is the
face of the Great stellated dodecahedron.

Fig. 11b: Extending the 12 faces of the Dodecahedron as in Fig. 11a, we obtain the
four stellations of the Dodecahedron listed in Fig. 11 a.

Fig. 12a: An incomplete stellation diagram
of the Icosahedron, representing some of the figures that can be built with a
small Zometool model. The inner Triangle
if the face of the Icosahedron, the Green triangle is a face of the
compound of five Tetrahedra and the outer triangle is a face of the
Great icosahedron. An intermediate figure where each face is composed of
three disjointed (blue) triangles, touching the face of the Icosahedron at its vertex, is
the self-dual Excavated dodecahedron (which is, therefore, another faceting of the Dodecahedron).
These are only four of the 59 stellations of the Icosahedron, some others were presented already in Fig. 7.

Fig. 12b:
Extending the 20 faces of the Icosahedron as shown above, we have
the four stellations of the Icosahedron mentioned above.

Fig. 13a: The stellation diagram
of the Rhombic dodecahedron built with Zometool. The inner diamond
if the face of the Rhombic dodecahedron.

Fig. 13b: The four stellations of the Rhombic dodecahedron. Each of the 12 faces of the Rhombic dodecahedron
has been extended along their planes as shown above.

Fig. 14a: The inner region of the
stellation diagram
of the Rhombic triacontahedron built with Zometool. The outer Rhombus is the face of the
Great rhombic triacontahedron. All other struts represent intersections of its
30 rhombic faces.

Fig. 14b: If, for each facial plane we include the complete set of struts and balls as in Fig. 14a,
then we obtain this model, which represents many of the
stellations of the Rhombic triacontahedron up to the Great rhombic triacontahedron (the outer shape).
As in Fig. 14a, every line represents the intersection of two faces of the Great rhombic triacontahedron.

Fig. 14c: Excluding most struts and connectors from the stellation diagram, we see the faces of some of
the more important stellations of the Rhombic triacontahedron. The inner red Rhombus is one of the 30 faces of the
Rhombic triacontahedron. The yellow Rhombus is one of the 30 faces of the
Medial rhombic triacontahedron.
The blue square is one of the 30 faces of the
compound of 5 cubes.
As in Fig. 14a, the outer Rhombus is one of the 30 faces of the
Great rhombic triacontahedron.

Fig. 14d: Extending the 30 faces of the Rhombic triacontahedron as in Fig. 14c, we obtain this model.
The four stellations can be found very easily since they are represented by different colours.
This model is consistent with the ``4 stellations'' theme set by the previous models.

For more on the latter models and instructions on how to build them, see my page on the many stellations of the Rhombic triacontahedron.

H. S. M. Coxeter, in the preface of ``Regular Polytopes".

The generalization of polygons in 2 dimensions and polyhedra in 3 dimensions to any number of dimensions is a polytope. I am particularly interested in 4-dimensional polytopes, the polychora, which are finite regions of 4-D space bound by polyhedral 3-faces, or cells.

Among an unknown number of uniform polychora, sixteen (again!) are regular: six are convex and ten are non-convex; the latter are known as the

Since all these models have a lot of important internal structure, there is no alternative to building them in Zometool: a paper model would hide the internal structure of the projection.

All of these rectified polychora have orthographic projections that can be depicted in the Zometool system.

Fig. 15a: Front row: Vertex-first projections of three convex regular polychora:
On the left is the simplest regular polychoron, the 5-Cell,
which is bound by 5 Tetrahedral cells and has 5 vertices, with Tetrahedral
vertex figures. This is the 4-dimensional analogue of the Tetrahedron.
In higher dimensions, the analogues are known as
Simplexes, all of them self-dual.
This is one of the few projections in this page where the "near" and "far" sides of the projections do not coincide.

At the centre is the vertex-first projection of the 16-cell, which is bound by
16 Tetrahedral cells and has 8 vertices with Octahedral vertex figures.
This the 4-D analogue of the Octahedron. The analogues in any dimension are known as
Orthoplexes.

On the right is the projection of its dual, the 8-Cell, more commonly known as the Tesseract.
This is bound by 8 Cubes and has 16 vertices with Tetrahedral vertex figures. This is the 4-D
Hypercube.

As one might expect, Tesseracts can fill 4-D space,
but more interestingly, the 16-cell can do that as well:
The vertex arrangement of this 16-cell honeycomb is known as the F_{4} lattice.
If a 3-sphere is centered in
each point of this lattice, the resulting arrangement is the densest possible
regular sphere packing in
4 dimensions, with kissing number 24.

In the row further back are the rectifications of these polychora (also, rectifications of the
particular projections in the first row).

On the left is the cell-first projection of
the Rectified 5-cell.
For each of the 5 Tetrahedra of the 5-cell, this has 5 rectifications
of the Tetrahedron, or Octahedra. Each vertex of the 5-cell was replaced
by its vertex figure, a Tetrahedron.
This is one of the 3 non-regular uniform polychora that has only regular cells,
these are known as a Semi-regular polychora.
In particular, this is a member of a multi-dimensional family of Semi-regular polytopes,
where the facets
are Simplexes and Orthoplexes, known as the
k_{21} polytope family,
where k is the dimension − 4. Thus the Rectified 5-cell is the 0_{21} polytope. More about this family below.
This is another of the projections in this page where the "near" and "far" sides of the projections do not coincide.

In the middle is a cell-first projection of the Rectified 16-cell. More about this object below.

On the right is tetrahedral cell-first projection of the Rectified tesseract. Each of the 8 Cubes of the Tesseract
was replaced with rectifications of the Cube, Cuboctahedra. Each of the 16 vertices of
the Tesseract was replaced by the Tesseract's vertex figure, Tetrahedra.
This is another case of a model where the "near" and "far" sides of the projections do not coincide: this is the reason why the model
displays two crossed Tetrahedra at the centre (the "Stella Octangula" design).

The two models on the left have pentachoric symmetry,
the other four share the hexadecachoric symmetry,
but one of them (the Rectified 16-cell, below) has a higher degree of symmetry.

Fig. 15b:
In Fig. 15a we displayed the vertex-first projections of the 16-cell and
Tesseract. Here we display, in the front row, their cell-first projections.
Behind them we display the rectifications of these polychora, specifically
rectifications of these projections. The projection of the rectified
Tesseract (top right) is different from that shown in Fig. 15a: Instead of
being centered on a Tetrahedron, it is centered on a Cuboctahedron. However,
the rectification of the cell-first projection of the 16-cell is identical to the
rectification of the vertex-first projection in Fig. 15a. This is because
both are centered on Octahedra. There is a deeper, and rather beautiful reason
for this, see Fig. 29.

This projection of the 16-cell is especially good for highlighting its 8
vertices separately. These represent half of the vertices of the Tesseract,
its dual polytope, i.e., the 16-cell is a ``Demi-tesseract'', the 4-D
Demi-hypercube
(the 3-D version, the Tetrahedron is a ``Half-cube'', see
the ``Stella Octangula'' model in Fig. 10).
This particular projection also depicts two superposed
16-cells that together have all the vertices of the Tesseract.

Note: the two models on the right are not permanently in my office.

Fig. 16: Left: Yet again, the Rectified 16-cell. For each of the Tetrahedral cells of the 16-cell,
this has their rectifications, 16 Octahedra. The 8 vertices of the 16-cell are here
replaced by the latter's vertex figures, also Octahedra. This is therefore a regular polychoron
bound by 24 Octahedra in total; it is
more commonly known as the 24-cell, or Polyoctahedron.
This polychoron has many interesting characteristics:
It is a self-dual polychoron with no analogue in any dimension other than 4.
Its 24 vertices are those of the Tesseract and the 16-cell combined, or the combination
of three 16-cells (since the 16-cell is a Demitesseract). A set of 3 16-cells
with the vertices of the 24-cell is a regular polychoron compound,
this is presented in Figs. 32a, b and c. Any model of the 24-cell will
also represent the dual of the compound of 3 16-cells, the regular compound of three Tesseracts. For more on this see Fig. 32d.
For more projections of the 24-cell, see Figs. 30a and 30b.

The 24-cell can fill 4-D space, in what is known as the regular Icositetrachoric honeycomb. This is dual to the 16-cell honeycomb mentioned in the caption to Fig. 15a.

Right: A cuboctahedral cell-first projection of the Rectified 24-cell. For each Octahedron of the 24-cell
the latter has 24 Cuboctahedra (the rectification of the Octahedron). For each
of the 24 vertices of the 24-cell, the Rectified 24-cell has a Cube (the vertex figure of the
24-cell). This polychoron has 96 vertices, one for each edge of the 24-cell.

**How to build**: Have a look at the Eusebeia page on the Rectified 24-cell. For this particular model, see the part on the "Cantellated 16-cell", for the pyritohedric projection, see the first part of the page.

Both polychora have icositetrachoric symmetry.

Fig. 17: This is an Icosahedral cell-first projection of a
convex uniform polychoron, the
Snub 24-cell.
This can be built from the Rectified 24-cell in Fig. 16 by diagonally bisecting all squares.
If the diagonals are chosen correctly, then each of the 12 vertices of the Cuboctahedron
now has 5 edges converging on it, i.e., it has been
transformed into an irregular Icosahedron. The Cubes have been transformed into
sets of 5 Tetrahedra, with only the central one being regular. Then we
shorten the diagonals of these former squares in order to make two regular
triangles. This generates one regular Icosahedron for each of the previous 24 Cuboctahedra,
and five regular Tetrahedra for each of the 24 previous Cubes, making a total of
120 Tetrahedra. This operation preserved the number of vertices, which is still 96.
Because all cells are regular, this is also a semi-regular convex polychoron.

**How to build**: Have a look at the
Eusebeia page on the Snub 24-cell.
Also recommended is David Richter's
page on the 24-cell and its snub.

Unlike the polychoron models shown above, this polychoron is neither regular nor a rectification, i.e., its Wythoff construction is very different from most polytopes in this page.
The vertices and edges of this model are a subset of those of the model of the 600-cell just below, i.e., this is a
diminished 600-cell.

Picture by Jason Wu.

Fig. 18: This is the vertex-first projection of a regular polychoron known as the 600-cell, or Polytetrahedron.
This is a 4-D analogue of the Icosahedron.

This polychoron can be obtained from the Snub 24-cell in Fig. 17
by adding on ``top'' of each of the latter's 24 Icosahedra
a 4-D ``Pyramid'' consisting of an Icosahedral ``base''
and 20 regular Tetrahedra as ``sides''. The 24 apices of these Pyramids have the same
arrangement as the vertices of a 24-cell. Together with the previous 96 vertices of the Snub 24-cell, they
add to a total of 120 vertices. The 120 Tetrahedra of the Snub 24-cell
are now joined by the 24 × 20 Tetrahedra = 480 Tetrahedra of the new
4-D ``Pyramids'', making a total of 600 Tetrahedral cells.
The apices of the new ``Pyramids'' have Icosahedral
vertex figures,
this is true for all other vertices as well because the 600-cell is regular.

**How to build**: see instructions in David Richter's
list of Zometool projects.

Picture by Jason Wu.

The high degree of symmetry of the 600-cell implies that there is nothing special
about the new 24 vertices added to the Snub 24-cell to form
the 600-cell. Just as the latter have the same arrangement as the vertices of the
24-cell, the previous 96 vertices can be decomposed into 4 groups of 24 vertices, each
also with the same arrangement as the vertices of a 24-cell. This means that
we can build a set of five
24-cells with the same vertex arrangement of the 600-cell. This is a self-dual
regular polychoron compound and is shown in Figs. 33a and 33b.
Furthermore, as mentioned in the caption of Fig. 16, each 24-cell can
be replaced by a set of 3 16-cells leaving the vertices unchanged.
Doing this for the compound of 5 24-cells results in a regular compound of 15 16-cells,
which will have the same vertices of the 600-cell.
A model of this is shown in Figs. 34a and 34b.

Another intersting aspect of this model: the outlines of the Icosahedra that were
in the Snub 24-cell are still visible. But apart from those, you will also be able to see
Dodecahedra and Icosidodecahedra in the model. Studying it further, you will also see
many flattened versions of those polyhedra.
Studying those will make it easier to understand and build some
of the models that come later.

Fig. 19: This is the cell-first projection of the dual of the 600-cell, the 120-cell, or Polydodecahedron. This
is bound by 120 Dodecahedra, it has 600 vertices with Tetrahedral vertex figures;
this is a 4-D analogue of the Dodecahedron.
This model is larger than the
set sold by Zometool as the hyperdo by φ, the
famous golden ratio, φ.

**How to build**: see instructions here.

Picture taken by Jason Wu.

Fig. 20: The icosahedral cell-first projection of the Rectified 600-cell. The 600 Tetrahedra
of the 600-cell are here replaced by their rectifications, which are Octahedra.
In the position of each of the 120 vertices of the
600-cell 120 Icosahedra (the vertex figure of the 600-cell) appeared.
Because all cells are regular, this is the last of the three semi-regular polychora.

**How to build**: After studying the perspective-flattened Icosahedra in the model of the 600-cell,
have a look at the
Eusebeia page on the Rectified 600 cell.
Also recommended is David Richter's page on the
rectified 600-cell.

This model has been disassembled.

Fig. 21: The icosidodecahedral cell-first projection of the Rectified 120-cell. The Dodecahedra of
the 120-cell are here replaced by their rectifications, Icosidodecahedra.
In the position of each of the 600 vertices of the
120-cell, 600 Tetrahedra (the vertex figure of the 120-cell) appeared.

**How to build**: Study the perspective-flattened Dodecahedra in the model of the 120-cell.
Make models of Icosidodecahedra with similar flattening. Then have a look at the
Eusebeia page on the Rectified 120 cell.

Picture taken by Jason Wu. This model has been disassembled.

The last 4 polychora have hexacosichoric symmetry.

Fig. 22: Another diminished 600-cell,
the Grand antiprism. This was the last uniform
convex polychoron to be discovered (in 1964) by John H. Conway and Michael Guy; they also proved that
there are no more undiscovered uniform convex polychora.

This is an anomalous uniform polychoron in the sense that, unlike all other polytopes
discussed above, it has
no Wythoffian construction.

Its structure also helps understanding the structure of the 600-cell, in particular the fact that the latter can be decomposed
in two disjoint perpendicular rings of 150 Tetrahedra each, separated by a Clifford torus
of 100 Tetrahedra with the two sets of 100 Tetrahedra that border that torus on each side. In the Grand Antiprism, both tetrahedral rings
have been removed and replaced with rings of 10 Pentagonal Antiprisms; in this model we're looking through one of these rings.

**How to build**: Study the model of the 600-cell in detail, then have a look at the
Eusebeia page on the Grand antiprism.

Picture by Aris Noutsos. Linked picture by Jason Wu.

It is important, before finishing, to note that although the models above include all the regular and ``semi-regular'' convex polychora, it includes only a small number of the convex uniform polychora. Some examples I have not built are in David Richter's list of convex uniform polytopes with pentachoric symmetry and his list of convex uniform polytopes with hexacosichoric symmetry. Many of the models based on the symmetry of the Tesseract and 24-cell cannot be built in Zometool because they require the construction of regular Octagons - which cannot be built in the Zometool system.

Their relations are depicted in Figures 26a and b below. Their cells and vertex figures can be read from Figure 31. In Fig, 26b, we can see that three of them - the Icosahedral 120-cell (the cells are the Icosahedra mentioned in the caption of Fig. 18), the Grand 120-cell (the cells are the Dodecahedra mentioned in the caption of Fig. 18) and the Great 120-cell (the cells are Great dodecahedra) - share the same edge arrangement of the 600-cell. This makes them analogues of the Great dodecahedron, which has the edge arrangement of the Icosahedron. The Great 120-cell is a particularly good example of this, since it has Great dodecahedra as cells; the latter's edges are those of the Icosahedra mentioned in the caption of Fig. 18.

Thus the Zometool model of the 600-cell shown in Fig. 18 also depicts the edge frames of the orthographic projections of these 3 Schläfli-Hess polychora!

Below are three models that represent the 7 remaining Schläfli-Hess polychora:

Fig. 23a: This model represents the vertex-first projection of two other regular
Schläfli-Hess polychora which share the same edge arrangement, the
Small stellated 120-cell
and the Great grand 120-cell.

**How to build**:
see instructions in
David Richter's dedicated page.

Fig. 23b: This is how it looks like in my office. Picture by Jason Wu.

As shown in the caption to Fig. 23c (later in this page), this model also represents
one of the two regular compounds of 25 24-cells and one of the two regular compounds of 75 Tesseracts.

Fig. 24a: This model represents the vertex-first projections of
four Schläfli-Hess polychora that share the same edge arrangement:
The Grand 600-cell,
the Great stellated 120-cell,
the Grand stellated 120
and the Great icosahedral 120-cell.

Fig. 24b: This is how it looks like in my office. Picture by Jason Wu.

According to David Richter's page on this
polytope, the edges in this model are images of the edges of the quasicrystalline projection of
Gosset's eight-dimensional
4_{21}
polytope, the largest finite member of the k_{21} polytope family mentioned above.
More about this family below.

**How to build**: Make a model of the 600-cell, but extend all internal edges:
there can be no broken lines. Then build a new,
outer set of vertices of the 600-cell, but increased in side by the Golden ratio,
as in Figure 36a (only a few of these will suffice). For each
new outer vertex, see what edges of the internal model point towards it,
then extend those edges to the outer vertex. Do this for a set of neighbouring vertices,
which will allow you to work out the intersections of those edges. Once this is done, apply
the same pattern to all outer vertices using icosahedral symmetry.
Note that, as in the previous model, there are several intersecting blue edges.
Because I wanted to make this a permanent addition to my office, I cut the necessary
number of blue struts with pliers.

Fig. 25a: The last of the Schläfli-Hess polychora, the most complex of the
16 regular polychora, the final stellation of the 120-cell:
The Great grand stellated 120-cell.
Here it is seen from a 5-fold symmetry axis.

Fig. 25b:
Here seen from a 3-fold symmetry axis.

This model can use 20 very long yellow struts, no longer sold by Zometool
(but easily found on eBay). These will be directly aligned with the 3-fold symmetry axis shown in this Figure. This saves 40 regular-sized struts and 20 balls and slightly improves the appearance of the model.

See also David Richter's page on this model.

**How to build**: Make a smaller version of the Small stellated 120-cell (in Fig. 23a), but with all internal edges extended - there can be no broken lines.
Then identify the equivalent vertices of the largest possible
Dodecahedron in the model, i.e., the outermost points along the 3-fold symmetry axes.
This set of vertices is the equivalent of the vertices of the inner Dodecahedron of the
120-cell. Now, based on this, build the remaining vertices of the 120-cell, at an
appropriate scale. Then, from each outer vertex, see what edges in the inner model
point towards it, and extent those edges until they touch the outer vertex.
Doing this for a set of neighbouring vertices will then allow you to figure out the
network of edge intersections. Once this is done, repeart for all other outer
vertices using icosahedral symmetry.
Note: This model suffers even more from the blue strut intersections that
appear in the previous two models. In this model, I omitted some of those intersections.

With this model, the list of regular polychora is complete!

Fig. 26a: Stellation relations between the 120-cell, 600-cell and the Schläfli-Hess
polychora; these provide an explanation of their names.
As in Fig. 5, the vertical scale indicates the
density and the two-sided gold arrows denote duality; note that the Great 120-cell and the
Grand stellated 120-cell are self-dual.
To a cell in a polychoron corresponds a vertex in its dual (the line from the centre
to the vertex is perpendicular to the 3-D plane of the cell), to a face in the polychoron corresponds
a perpendicular edge in its dual going through the face's centre, to an edge in the polychoron corresponds a face in its dual in a perpendicular plane and to a vertex in the
polychoron corresponds a cell in its dual.

The dark blue arrows denote edge stellation, which has the same meaning as in 3-D.
In the case of the 120-cell, this operation produces the Small stellated 120-cell.
Each of the 120 Dodecahedra of the 120-cell was edge-stellated into a Small stellated
dodecahedron (Fig. 4); the latter has only 12 vertices (one for each face of
the Dodecahedron) arranged as in the Icosahedron.
Likewise, the Small stellated 120-cell has only 120 vertices - one for each cell of the
120-cell, arranged as in the 600-cell.
By the rules of duality, the dual polychoron, the Icosahedral 120-cell, will also
have 120 cells and 120 vertices.

The light blue arrows denote greatening; as in 3-D this means replacing a face by an
identical, larger one in the same plane. Finally, the green
arrows denote a new operation for polychora, aggrandizing (replacing cells by
identical larger ones in the same 3-d ``plane'').

Analogously to the 3-D case, none of these operations changes the number of cells or
their 3-d ``planes''.
Therefore, all stellations of the 120-cell (the polychora on the ``cubic'' chain
starting on the 120-cell) must have 120 cells as well. As explained 2
paragraphs above, this is also true for the Icosahedral 120-cell, so it is also
true for the latter's stellation, the Great icosahedral 120-cell.
The Grand 600-cell is the only stellation of the 600-cell,
so it is the only Schläfli-Hess polychoron with 600 cells. This
makes it the 4-d equivalent of the Great Icosahedron in Fig. 4.
Adapted from Conway, Burgiel and Goodman-Strauss (see references below).

Fig. 26b: Faceting relations between the 120-cell, 600-cell and the Schläfli-Hess polychora.
As in Fig.5 these operations can be seen as the duals of the stellation operations
in Fig. 26a, i.e., they are like a mirror image of the latter.

Since none of the stellation operations changes the number and hyperplane
of the cells, all faceting operations preserve the vertex arrangements, as in 3 dimensions.
Therefore, we see straight away that the eight polychora in the cubic chain starting on the
600-cell (the duals of eight polychora in the stellation chain of the 120-cell shown in Fig. 26a)
have its vertex arrangement, i.e., they are all facetings of the 600-cell.
As mentioned in Fig. 26a, this is also true for the Small stellated 120-cell, so its faceting,
the Great grand 120-cell, must also have the vertex arrangement of the 600-cell.

The Great grand stellated 120-cell, one of the many stellations of the 120-cell,
is the only regular faceting of the 120-cell, i.e., it is the only Schläfli-Hess
polychoron with 600 vertices. It is the dual of the Grand 600-cell, one
of the many facetings of the 600-cell that is its only regular stellation.
This makes the Great grand stellated 120-cell a 4-D analogue of the
Great stellated dodecahedron (see Fig. 4), which it has as cells.

We now describe the individual faceting operations. The solid red and gold lines
are equivalent to: finding dual + edge stellating + finding dual. Since the edge
stellation preserves
the edge directions, the dual faceting operation preserves the
face arrangements,
which also imply the same edge arrangement.
The polychora at the ends of these lines are not identical because their cells differ.

The dashed lines are equivalent to find dual + greaten + find dual.
Since greatening preserves the type of face and its plane, the dual faceting operation preserves the edge arrangement.
Since Zometool models only depict edge arrangements, this conservation law is what defines
how the polychora are represented:
The 4 polychora in the red circuit can be depicted by the model of the 600-cell (Fig. 18),
the 2 polychora in the purple line are depicted by the model of the Small stellated 120-cell (Figs. 23a and b) and
the 4 polychora in the gold circuit can be depicted by the model of the Grand 600-cell (Figs. 24a and b).
The Zometool models of the 120-cell (Fig. 19) and the Great grand stellated 120-cell
(Figs 25a and b) depict only those polychora.

The solid blue lines are equivalent to: find dual + aggrandize + find dual.
Since aggrandizing preserves the cell type, the dual faceting operation preserves
the vertex figure.
The light blue lines show that each polychoron in the red family has
a faceting in the yellow family with exactly the same vertex figure.
The dark blue line shows that the only faceting of the 120-cell, the
Great grand stellated 120-cell, also shares the former's vertex figure.

Johannes Kepler

We present below Zometool models of the Coxeter-Dynkin diagrams for the polytopes shown above. In the Zometool system, the yellow struts connect to the triangular holes in the connectors (the balls), they here represent the 3-symmetry branch in the C-D diagrams (which have no attached number because they are so common). The blue struts connect to rectangular holes in the connectors, they represent the ``4'' branches in the C-D diagrams where they appear. The red struts connect to the pentagonal holes in the connectors, they represent the ``5''-branches in the C-D diagrams where they appear. The half-length green struts connect to the pentagonal holes, but they have a twist and are only half length of a regular green, for that reason they symbolize here the ``5/2''-branches in the C-D diagrams where they appear.

The diagrams with only white balls represent a Coxeter group, which is akin to a set of mirrors in a Kaleidoscope. In the case of polyhedra, these can be thought as dividing a spherical surface in a set of identical Schwarz triangles. In the case of polychora, these can be thought as dividing a hyper-spherical surface in a set of identical Goursat tetrahedra. Identical diagrams with only red balls at opposite ends represent dual polytopes.

Regular polytopes and their rectifications can then be thought as reflections of one of the

Fig. 27: These are the C-D diagrams of the regular polygons
used in the polychora above, plus their generating groups.
All these graphs are left-right symmetric, this means that
all regular polygons are self-dual. The number of such diagrams
is, of course, infinite.

Fig. 28: These are the C-D diagrams
of the regular and quasi-regular polyhedra displayed above, plus their generating
groups. On the left column we have the graphs for the groups,
in the middle column we have the convex polyhedra, and
in the right column we have the star polyhedra.

These diagrams include the polygonal diagrams in Fig. 27,
such polygons are thus a part of the polyhedron.
For instance, for the Cube, the only polygon graph
that can be built with the red ball is the Square. However,
for the Icosidodecahedron, we can form the graphs of the
Pentagon and the Equilateral triangle with the red ball (since the graph can
be read in both directions); thus the polyhedron is bound
by both types of polygons. Two neighbouring white nodes
indicate a regular vertex figure: from this, we can see immediately
that the vertex figure of the Cube is a regular triangle.

At the start of the page we said that regular and quasi-regular
polyhedra share the same Kaleidoscopic Wythoff construction.
This fact is evident in the C-D diagrams by the fact that all
polyhedron graphs have only one red ball, i.e., they are reflections
of vertices of their Schwarz triangles. Other Wythoff constructions, which reflect points in the edges
or even faces of the Schwarz triangles to create many uniform polyhedra,
would require more than one red ball.

An important point to re-emphasize is that a particular polyhedron
(like the Octahedron) can be represented by different
diagrams. This is a reflection of the fact that the same polyhedron
can be produced from different symmetries. These polyhedra have
several other C-D diagrams, we present here those where only
one red ball is needed; which directly implies regularity or
quasi-regularity.

_{3} graph is symmetric, therefore the Tetrahedron can be
generated with the red ball at either end. This means that
the Tetrahedron is delf-dual.

Fig. 29: These are the C-D diagrams of the
convex polychora presented above, plus their generating groups.

On the left we have most of the group graphs.
In the middle we have the convex polychora displayed above.
These include as sub-sets the polyhedral graphs in the
middle column of Fig. 28.
For instance, in the 16-cell, the only polyhedral graph
that can be built with the red ball is the Tetrahedron,
therefore the 16-cell only has Tetrahedra, and is therefore
regular. In the case of the rectified 5-cell, however,
we can build the graphs of the Octahedron and the Tetrahedron
from the red ball; this means that that polychoron
is bound by both types of polyhedra.
Three neighbouring white nodes indicate a regular
vertex figure (which happens, of course, only for regular
polychora), with the equivalent of the red ball next to the
actual red ball. Doing this for the 600-cell, for instance,
we see that the vertex figure is an Icosahedron.

Most (but, unlike in Fig. 28, not all) of the polytope graphs presented here have the same
Wythoff construction,
i.e., they have one red ball. The exceptions are the diminished 600-cells:
the Snub 24-cell (see Fig. 17), which has two green balls (indicating rotational
but not reflexive symmetry) and the Grand antiprism. The latter does not appear
in this Figure because (as mentioned in the caption to Fig. 22) it has no Wythoff construction.
Many other convex uniform polychora are possible with the use of more red balls,
but building all of them requires many parts, as one can see in
David Richter's H4 page.

Studying these diagrams, we can see that the process of
rectification of a regular polychoron with X-type of cell
and Y-type of vertex figure generates a new polychoron
for which the cells are rectified Xs (as many as the previous
number of cells) and Ys (as many as the previous number of vertices).
The number of vertices will be the same as the number of
edges in the polychoron before.

Again, almost all of these polychora can be represented by
multiple C-D diagrams; those presented here are those that require
only one red ball.
Note that the 24-cell is represented by 3 different
diagrams in the figure, and the 16-cell by two. Some of these extra
diagrams appear in the right column, we have, on top,
the Demi-hypercubic
group D_{4}.
In 4 dimensions, this type of symmetry does not yet produce
new polytopes, this starts happening only in 5 dimensions.
However, it has some interesting consequences, one of them
being Triality.

This concept deserves a detailed explanation. In the case of duality in 3 dimensions,
one can, by the definition of the meaning of duality,
scale two concentric dual polyhedra in such a way that each edge from
a polyhedron meets another (perpendicular) edge from the dual polyhedron
at a point that is in the middle of both (the midpoint).
Those two edges form a plane that is perpendicular
to a third line joining the midpoint to the centre of those
polyhedra. Rectifying those two dual polyhedra results in the same rectified
polyhedron.

In the case of Triality in 4 dimensions, the situation is very similar,
except that the perpendicular edges of *three* concentric ``trial'' polychora
(16-cells for the only regular case) meet at
their midpoints. These edges are in a 3-D ``plane'' that is itself perpendicular to
a fourth direction, the line joining those midpoints to the centres of the trial polychora.
Rectifying all three polychora results in the same rectified polychoron,
the regular case being the 24-cell.

The same applies to projections: if we pick three ``trial'' projections of the
16-cell and rectify them, we obtain an invariant projection
of the 24-cell. In this page, we show a triad of such trialities.
The first we met already in Figs. 15a and 15b, triality
is the reason for the identical rectifications of the vertex-first and
cell-first projections of the 16-cell. The other two are shown in
Figs. 30a and 30b.
This shows the predictive power of the C-D graphs.

Fig. 30a:
Three edge-first projections of the 16-cell, with the central edges
of the projections loosely aligned along 3 perpendicular orthogonal axes in 3-d space.
Rectifying all three projections results in the same projection of
the 24-cell, which is shown in the centre. This is its vertex-first
(or ``pyritohedric'')
projection, the dual of the cell-first projection in Figs. 15a and 15b.

Fig. 30b:
Bottom: The three ``prismatic'' projections of the 16-cell.
Rectifying all three projections results in the same projection of
the 24-cell, also known as its ``prismatic'' projection, this is shown by the larger model above.
One of the beauties of this model is that it shows all vertices,
edges, faces and cells separately, whithout superpositions.

For a detailed explanation of these models, see David Richter's
Triality with Zometool page.

Fig. 31: These are the C-D diagrams of the
Schläfli-Hess polychora presented above (on the left column),
plus those of their rectifications (on the right column).
I have built models for all polychora on
the left, but not for their rectifications (for lack of space, time and money...),
except for one or two (see below).

These also include the star polyhedra diagrams in the right
column of Fig. 28. From these diagrams, we can see, for instance,
that the Small stellated 120-cell
is bound by Small stellated dodecahedron cells (the only polyhedral
graph that can be built from the red ball) and that this
has a Dodecahedral vertex figure. Thus its dual, the Icosahedral 120-cell,
has Icosahedra as cells, and Great dodecahedra as vertex figures.
We can also see that, following the logic of rectification,
the Rectified small stellated 120-cell has Dodecadodecahedra
and Dodecahedra as cells, and that the Rectified icosahedral 120-cell
has Icosidodecahedra and Great dodecahedra as cells.

Note that the edges of the latter rectified polychoron are
identical to those of the Rectified 600-cell (Fig. 20); thus
both can be represented by the same Zometool
model. The identical rectification is a
consequence of the conservation laws in Fig. 26b: the rectifications of
two polytopes that share the same edge arrangement will necessarily share the
same vertex arrangement, since the vertex of the rectification is the
middle point of the edge of the original polytope.
The rectifications of two polytopes that
additionally share the same face arrangement (like the 600-cell and
the Icosahedral 120-cell) will necessarily share the
same edge arrangement.

The symmetry of graphs for the Great 120-cell and the Grand-stellated
120-cell indicates that these are, as remarked above, self-dual.

Johannes Kepler

The models below show some of the regular polychoron compounds. As in the case of the regular polyhedron compounds, these can be seen as important facetings of the regular polytopes. They also illustrate the fact that some of the polychoron symmetry groups are sub-groups of others.

The concept of triality described above allows a better understanding of the first object we discuss below, the compound of three 16-cells. We present three projections of this compound, which result directly from stellating (and/or faceting) the three projections of the 24-cell in Figs. 16, 30a and 30b.

Fig. 32a: Superposing the 3 orthogonal 16-cells in Fig. 30a, we obtain, on the right,
a regular polychoron compound
with three 16-cells. This is the first stellation of the
24-cell; this particular projection results from stellating the pyritohedric projection of the
24-cell on the left. Since the latter has the Rhombic dodecahedron as its outer envelope,
this projection has, as its outer envelope,
the
first stellation of the Rhombic dodecahedron; the latter is also
known as ``Escher's polyhedron''.

Each of the vertices of the 24-cell is transformed into the mid-point of three
edges of the compound of 3 16-cells (remember the triality!), these are represented in this and
the following figures (32b and 32c) by the black balls, the real vertices are represented in these
figures by the white balls. The green balls in this model represent 3-edge intersections
that coincide with a real vertex of the 16-cells, this happens only in this model.

An inspection of the model will show that the real vertices have the same arrangement
as the vertices of the cell-first projection of the 24-cell (seen on Fig. 32b
on the left), which is the dual of the pyritohedric projection of the 24-cell.
This implies that (as mentioned in the caption of Fig. 16) the vertices of
the regular compound of three 16-cells are arranged as the vertices of a 24-cell.

Fig. 32b: Combining one vertex-first
projection of the 16-cell in Fig. 15a with two complementary
superposed cell-first projections of the 16-cell in Fig. 15b, one
obtains, on the right, a different projection of the compound of three 16-cells. This projection
is the stellation of the cell-first projection of the 24-cell on the left. Since the latter
has a Cuboctahedral envelope; its stellation's envelope is a
composite of a Cube and a Octahedron.
The real vertices of this projection coincide with those of
of the pyritohedric projection of the 24-cell (on the left in Fig. 32a), but have,
in this model, twice the separation. This means that although the dual of
the 24-cell is also a 24-cell, one of the dual pairs is larger (or smaller) than the
other by the square root of 2.

This model shows very clearly that each of the individual Octahedra of the 24-cell was
stellated into a ``Stella Octangula'', as in Figs. 10a and 10b.
Therefore, the compound of three 16-cells can also be seen as a compound of 24 ``Stella Octangula'',
with a total of 48 Tetrahedral cells.

Fig. 32c: Combining the three prismatic projections of the 16-cell in Fig. 30b one
obtains, on the right, the prismatic projection of the compound of three 16-cells.
This is the stellation of the prismatic projection of the 24-cell on the left, which also
appeared in Fig. 30b.
The red balls in both models are edge intersections that appear because of the projection; they are
not real edge intersections in 4 dimensions.
The real vertices of the compound of three 16-cells (white balls) have the same arrangement
of the dual of the prismatic projection of the 24-cell, a projection of the 24-cell
that cannot be built in the Zometool system.
Both models are built using very long struts, which are no longer sold by Zometool.

**How to build**: Check
David Richter's dedicated page, which also provides many more details on this model.

One of the advantages of the prismatic projection of the compound of three 16-cells is
that is shows all 48 real and false vertices of the compound separately - no superposed vertices here.
All edges, faces and cells are also shown in the model.
These real and false vertices are the same as the vertex arrangement of the dual configuration of 24-cells;
this represents the 48
root vectors of the F_{4} group.
Like the 24-cell, this is a truly exceptional object.

Fig. 32d:
On top right we see the pyritohedric projection of the compound of 3 16-cells.
On lower right, we see one of the components of the latter, the edge-first projection
of the 16-cell. Its dual is the face-first projection of the Tesseract (lower left).

The dual of the compound of three 16-cells is another regular compound, with three
tesseracts. Amazingly, a projection of that regular compound (the dual of
the pyritohedric projection of the compound of 3 16-cells) is well represented by the
cell-first projection of the 24-cell (above left).
With some attention, you might discern the 3 face-first Tesseracts in that model.
This means that all projections of the 24-cell in Figs. 32a, b and c are also projections
of the compound of 3 Tesseracts. As an example, the pyritohedric projection of the
24-cell looks exactly like a superposition of two complemetary vertex-first and one
face-first projections of the Tesseract in Figs. 15a and 15b.

Fig. 33a: With five 24-cells (one in pyritohedric projection, as in Fig. 30a, and four
in prismatic projection, as in Fig. 30b), we obtain a self-dual
regular polychoron compound.
In this picture, we're looking at its 3-d projection through a genuine three-fold symmetry
axis. This compound has 5 × 24 = 120 vertices, which happen to have the same arrangement
as the 120 vertices of the 600-cell in Fig. 18, which implies that this compound
is a faceting of the 600-cell.
This illustrates the fact mentioned in the caption of that figure that the vertices
of the 600-cell can be decomposed in five sets, each with the same arrangement as the
vertices of a 24-cell. The edges of this model are a sub-set of the edges of the
Small stellated 120-cell in Figs. 23a and 23b.

Fig. 33b: The regular compound of five 24-cells, now seen through a five-fold
``Ghost symmetry'' axis.

Note that since the edges and vertices of the compound of three Tesseracts
coincide with those of a 24-cell, the model above also represents another regular compound,
one with 15 Tesseracts, also a faceting of the 600-cell. In that case, each of the 120 vertices is shared by
two Tesseracts, instead of one 24-cell.

See detailed explanation of this model in
David Richter's dedicated page,
which includes a part count.
Here we're building this model on a φ smaller scale than the model in David Richter's
page. This has an interesting implication: If we can find some
of the very long old struts no longer manufactured by Zometool (12 very long reds, 12 very
long yellows), we can use each of them to replace a combination of two struts and one ball
where the ball is not strictly necessary (i.e., a ball where there is no intersection with
other edges). Doing this, we can save 48 regular-sized struts and 24 balls compared to the
part count in David Richter's page, and improve the appearance of the model.

Fig. 34a: Combining the pyritohedric projection of the compound of 3 16-cells (in Fig. 32a)
with four prismatic projections of the compound of 3 16-cells (in Fig. 32c), we obtain
the dual of the compound of 15 Tesseracts in Figs. 33a and b, the (also regular) compound of fifteen
16-cells. This is also the stellation of the compound of five 24-cells in Figs. 33a and b.
Here we see it through the 3-fold symmetry axis.

Each compound of 3 16-cells has the same vertices as a 24-cell, thus the vertices of this set
of 15 16-cells (arranged in 5 groups of 3 16-cells) are arranged as the vertices of the
compound of 5 24-cells, which is the same vertex arrangement of the 600-cell. This implies
that this is also a faceting of the 600-cell. Interestingly, in this
projection they are not arranged as the vertices of the projection of the 600-cell in
Fig. 18, but as a sub-set of the 600 vertices of the 120-cell in Fig. 19.
This compound can also be seen as a compound of 120 ``Stella Octangula''.

Fig. 34b: The compound of 15 16-cells, here seen through a 5-fold ``ghost symmetry''
axis.

See also David Richter's dedicated page,
which has a detailed description and part count.
As in the model of the compound of 5 24-cells, if we can find some of the very long old struts
(in this case, 48 very long reds, 120 very long yellows and 72 very long blues),
we can save 480 regular-sized struts and 240 balls compared to the
part count in David Richter's page, and greatly improve the appearance of the model.

Fig. 33c: Rectifying the compound of 15 16-cells, we produce three superposed copies of the
compound of 5 24-cells. As in Fig. 33b, we're looking at the model through one of its
ghost symmetry axes. However, in this photo the strut colors are not as obvious, so
the model resembles even more the model of the Small stellated 120-cell
in Figs. 23a and 23b.

As remarked above, the edges of this model are a sub-set of the edges of the
Small stellated 120-cell in Figs. 23a and 23b, while the vertices
have the same arrangement as the latter (which are the same as the 600-cell).
For each axis of ghost symmetry, we can superpose four other sets of five 24-cells,
each set rotated relative to the previous by 72 degrees around that axis.
The result is in the picture below:

Fig. 23c: This is another regular compound, one of the pair of dual compounds that has
25 24-cells. In this compound the 600 vertices still have the same arrangement as
the 600-cell; i.e., they appear in
120 unique points, with each point representing the vertices of five different 24-cells.
This implies that this compound is also a faceting of the 600-cell.
The 96 × 25 = 2400 edges will twice cover be the full set of 1200 edges of
the Small stellated 120-cell, i.e., each edge of the Small stellated
120-cell is shared by two 24-cells.
Thus the Zometool model of this compound of 25 24-cells is also the model of the
Small stellated 120-cell in Figs. 23a and 23b!

Again, because the edges and vertices of the compound of three Tesseracts
coincide with those of a 24-cell (with each vertex shared by two Tesseracts),
this model has the same vertices and edges as one of the two regular
compounds of 75 Tesseracts! This means that this model also represents
one of these compounds of 75 Tesseracts, the one where each of the 120 vertices
(arranged as those of the 600-cell, of which the compound must be a faceting)
is shared by 10 Tesseracts.

With relatively few models, we have built projections of seven of the regular polychoron compounds:

- Three different projections of the compound of 3 16-cells (Figs. 32a, b and c). These are at the same time facetings and stellations of the 24-cell.
- Three different projections of the compound of 3 Tesseracts (identical to the three projections of the 24-cell in Figs. 32a, b and c). This is the dual of the compound of 3 16-cells. Also a faceting of the 24-cell.
- The self-dual compound of 5 24-cells (Figs. 33a, b and c), a faceting of the 600-cell.
- The compound of 15 Tesseracts (identical to model of the compound of 5 24-cells in Figs. 33a, b and c), also a faceting of the 600-cell.
- The compound of 15 16-cells (see Figs. 34a and b), another faceting of the 600-cell, this is the dual of the previous compound of 15 Tesseracts and a stellation of the compound of 5 24-cells.
- One of the two dual compounds of 25 24-cells (identical to the model of the Small stellated 120-cell, see Fig. 23c), this one also faceting of the 600-cell.
- One of the two compounds of 75 Tesseracts (identical to the model of the compound of 25 24-cells, see also Fig. 23c), this one also a faceting of the 600-cell.

Some of the other compounds can also be built with Zometool. One example is one of the two compounds of 75 16-cells (see David Richter's page on that compound). This can be obtained from the compound of 15 16-cells using the same method we used to derive the compound of 25 24-cells from the compound of 5 24-cells: make 4 more copies and rotate them around the ghost symmetry axis. Therefore looking at the projection of the compound of 75 16-cells from its real 5-fold symmetry axis will be similar to the view of the projection of the compound of 15 16-cells along its ghost symmetry axis (shown in Fig. 34b). Unlike most compound models we have shown above, that latter is a faceting of the 120-cell.

I might do that model some other time. It is clear, however, that my office won't have the space for all those models.

Johannes Kepler

What happens at dimensions higher than 4?

The only regular polytopes are the Simplexes (generated by the A

In this way, one comes to appreciate the fact that a few of the symmetries shown above, like the Icosahedral (H

There are other interesting symmetries in higher dimensions. There is one more infinite family of uniform polytopes that has been thus far hidden: the Demi-hypercubes, generated by the D

Fig. 35: C-D diagrams for some of the higher-dimensional polytopes.
In the centre we see the infinite Demi-hypercubic family. All polytopes of
this family in 3 and 4 dimensions are also generated by the B_{3} and B_{4} groups.
In 5 dimensions, the D_{5} family starts generating unique symmetries that
are not present in the A_{n} or B_{n} families.

We also see the k_{21} family evolving along the diagonal.
This ends at 8 dimensions, with the 4_{21} polytope.
The next member of the family is an infinite tesselation filling
8-dimensional space.

In 6 dimensions, the k

In seven dimensions, the semi-regular 3

Finally, in eight dimensions, the semi-regular 4

That's it! The family ends, because its next member (still in eight dimensions!) is the infinite 5

Thus, one comes to the realization that the E6, E7 and E8 are also exceptional objects - rare jewels among the infinite geometric treasures we have just contemplated.

Fig. 36a: A Zometool model of the 4_{21} polytope.
The 240 vertices project here as the vertices of two concentric 600-cells,
with one of them being larger than the other by a factort of φ.
It is not possible to project all the edges into a 3-D Zometool
model, so we must choose a sub-set. In this case, we chose the edges
of the projections of the two concentric 600-cells, exactly as in
David Richter's model.
Here we can see that projecting higher-dimensional figures in three dimensions
leads to a concentration of vertices and edges near the centre.

This model required many old very long struts, no longer manufactored by Zometool:
120 very long yellows, 120 very long blues, and 60 very long reds.
Alternatively, the model can be made on a smaller scale.

Fig. 36b: An orthographic projection of the 4_{21} polytope in 3-D space, now with all the edges represented. This model is laser-engraved in glass.

Fig. 37: Print on my door: The orthographic projection of the 8-dimensional
4_{21} polytope onto the Coxeter
plane where its projection has maximal symmetry.
This 2-D projection highlights even more the concetration of vertices
towards the centre,
As its 240 vertices represent the
root vectors of the
simple
Lie group
E_{8},
the polytope is sometimes referred to as the ``E_{8} polytope''.
Using a complex number coordinate system, it can also be constructed as a 4-dimensional
regular
complex polytope known as
the Witting polytope.

Image by Claudio Rocchini (Own work), via Wikimedia Commons.

That's not the end of the fun, though. That has just started...

Consider the 24-dimensional Leech Lattice, where each sphere ``kisses'' 196560 neighbours, and provides the most compact sphere packing in that dimension! The number of symmetries in this lattice is:

8 315 553 613 086 720 000.

Or consider the Monster group, which can be represented by a polytope in 196883 dimensions! The number of its symmetries is:

808 017 424 794 512 875 886 459 904 961 710 757 005 754 368 000 000 000,

which is about 6000 times the number of atoms on Earth. As John H. Conway has said, we've only started scratching the surface of the laws of symmetry!

- ``Regular Polytopes'' by H. S. M. Coxeter. This is the book for people who want to understand regular polyhedra and regular polytopes. If you want to go overboard, then get ``Regular Complex Polytopes".
- ``The Fifty-Nine Icosahedra" by H. S. M. Coxeter, P. du Val, H. Flather and J. F. Petrie. A charming little book on the stellations of the Icosahedron.
- ``Mathematical models", by H. Martyn Cundy, A. P. Rollett. This is a very nice but inexpensive book that includes most of the paper models in my office, and much besides polyhedra.
- ``Polyhedron Models", ``Dual Models and ``Spherical Models" by Magnus Wenninger. These detail methods for building a very large number of polyhedron and related models, particularly uniform polyhedra.
- ``Zome Geometry: Hands-on Learning with Zome Models" by George W. Hart. This is a very nice introduction to the Zometool system.
- ``The Symmetries of Things'', by John H. Conway, Heidi Burgiel and Chaim Goodman-Strauss. This is a very fun, deep and extremely well-illustrated book on everything symmetric, with a very modern approach.

- The most valuable resource for anyone in the first stages of learning any topic must surely be Wikipedia, one of the best things to happen in the Internet age. I link to it extensively in this page.
- David Richter's page, which includes a very nice list of Zometool projects. Many of the models in my office (600-cell, first stellation of the 120-cell and others) were built following directly the instructions in these pages - I learned a lot building those models! Most others were inspired by models that appear in these pages. A big Thank You to David for the very inspiring and educational resource!
- George Hart's page. From his beautiful site and its links you may explore the whole polyhedral universe.
- Eusebeia 4-D visualization. This is very useful for figuring out how to build Zometool projections of 4-D regular and uniform polychora.