In 1992, while teaching at the
Technical University of Ilmenau, I gave a three-semester course on the use of
Mathematica. I am a theoretical physicist by training, so the graphics component was just one of the not-so-important parts of the system for me at the time. Calculating integrals and minimizing functions for many-parameter variational wave functions of semiconductor nanostructures in very high magnetic fields was much more on my mind.
But the students asked me to cover graphics in depth too, so I did. The cover picture of the Mathematica 2 book had a
hyperbolic dodecahedron on it (the Version 1 book has a graphic of the
Riemann zeta function along the critical strip).
The hyperbolic dodecahedron is quite symmetric and has the same symmetry group as a regular
dodecahedron. It has a natural 120-fold symmetry (12 equivalent faces, each being a pentagon made from 10 equivalent pieces). Each one-tenth of a face just has a few polygons. By using the full symmetry group of the dodecahedron, constructing the
tesselation used on the cover was relatively easy.
Starting with a regular dodecahedron with appropriately subdivided faces, one just has to extend the vertices outwards (or press the face centers inwards) to obtain a hyperbolic dodecahedron. I showed the construction in the lecture (a nice mixture of geometry, matrix algebra, equation solving and graphics itself).
Little did I know at that time that the force of the hyperbolic dodecahedron would be with me for the next 15 years.