One of the nice things about inversive limit sets is that they typically are deviations from a sphere (e.g. here) so it is tempting to think they could be used to define a global landscape such as mountains, craters and hills on a planet or moon. To get the variety you can use the inversive substitution rules approach of my recent post, which was based on an octahedral configuration of six spheres. You then stat with a spherical limit set and switch to varied configurations. There are a wide variety of configuration but in this post I'll consider only distortions, meaning the same connectivity but different placement and size of the spheres.
The problem with the octahedral vertices is that there is only 1 degree of freedom in distorting from a sphere. This gives you a cratered shell-shell all the way to the lumpy tree-tree seen in the recent post, but no others.
For the tetrahedral spherical limit set it is worse, there are no degrees of freedom. You must stay as a sphere.
For the cubic arrangement there are also no degrees of freedom. The faces must stay planar.
For the dodecahedral arrangement there is no connectivity diagram possible that covers the whole face, which means it does not generate a surface.
That leaves only the icosahedral arrangement among the most symmetrical of spherical limit sets. Its limit set is shown on the right:
Fortunately this does allow at least four degrees of freedom in transitioning from spherical. In these examples the top six spheres remain fixed to allow the transition. I'll give the degrees of freedom parameter names:















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