Fractals and Steiner chains

I recently came across this nice animated gif of a fractal based on a Steiner chain, due to Eric Martin Willén. I immediately wanted to replicate it.

Make Steiner chains easily

First, how do you make a Steiner chain? It is easy using inversion geometry. Just decide on the number of circles tangent to the inner circle (n). Then the ratio of the radii of the inner and outer circle will be r/R = (1-\sin(\pi/n))/(1+\sin(\pi/n)). The radii of the circles in the ring will be (R-r)/2 and their centres are located at distance (R+r)/2 from the origin. This produces a staid concentric arrangement. Now invert with relation to an arbitrary circle: all the circles are mapped to other circles, their tangencies preserved. Voila! A suitably eccentric Steiner chain to play with.

Since the original concentric chain obviously can be rotated continuously without losing touch with the inner and outer circle, this also generates a continuous family of circles after the inversion. This is why Steiner’s porism is true: if you can make the initial chain, you get an infinite number of other chains with the same number of circles.

Iterated function systems with circle maps

The fractal works by putting copies of the whole set of circles in the chain into each circle, recursively. I remap the circles so that the outer circle becomes the unit circle, and then it is easy to see that for a given small circle with (complex) centre z and radius r the map f(w)=(w+z)r maps the interior of the unit circle to it. Use the ease of rotating the original concentric ring to produce an animation, and we can reconstruct the fractal.

Done.

Except… it feels a bit dry.

Ever since I first encountered iterated function systems in the 1980s I have felt they tend towards a geometric aesthetics that is not me, ferns notwithstanding. A lot has to do with the linearity of the transformations. One can of course add rotations, which cheers up the fractal a bit.

But still, I love the nonlinearity and harmony of conformal mappings.

Inversion makes things better!

Enter the circle inversion fractals. They are the sets of the plane that map to themselves when being inverted in any and all of a set of generating circles (or, equivalently, the limit set of points under these inversions). As a rule of thumb, when the circles do not touch the fractal will be Cantor/Fatou-style fractal dust. When the circles are tangent the fractal will pass through the point of tangency. If three circles are tangent the fractal will contain a circle passing through these points. Since Steiner chains have lots of tangencies, we should get a lot of delicious fractals by using them as generators.

I use nearly the same code I used for the elliptic inversion fractals, mostly because I like the colours. The “real” fractal is hidden inside the nested circles, composed of an infinite Apollonian gasket of circles.

Note how the fractal extends outside the generators, forming a web of circles. Convergence is slow near tangent points, making it “fuzzy”. While it is easy to see the circles that belong to the invariant set that are empty, there are also circles going through the foci inside the coloured disks, touching the more obvious circles near those fuzzy tangent points. There is a lot going on here.

But we can complicate things by allowing the chain to slide and see how the fractal changes.

This is pretty neat.

 

My Newtonmass Fractal

doubleshphere

I like the hyperbolic tangent function. It is useful for making sigmoid curves for neurons and fitting growth rates, it enables a cute minimal surface. So of course it should be iterated to make fractals! And there is no better way to celebrate Newtonmass than to make fractals!

As iteration formula I choose z_{n+1} = f(z_n) = \tanh(cz_n) , where c is a multiplicative constant. Iterating some number like 1 and plotting its fate produces the following “Mandelbrot set” in the c-plane – the colours here do not denote the time until escape to infinity but rather where in the complex plane the point ended up, as a function of c. In a normal Mandelbrot set infinity is an attractive fixed point; here it is just one place in the (extended) complex plane like any other.

"Mandelbrot set" for the hyperbolic tanh function tanh(cz).
“Mandelbrot set” for the hyperbolic tanh function tanh(cz).

The pinkish surroundings of the pattern represent points attracted to the positive solution of z=\tanh(cz). There is of course a corresponding negative solution since tanh is antisymmetric: if z is an attractive fixed point or cycle, so is -z. So the dynamics is always bistable.

Incidentally, the color scheme is achieved by doing a stereographic projection of the complex plane onto a sphere, which is then fitted into the RBG cube. Infinity corresponds to (0.5,0.5,1) and zero to (0.5,0.5,0) – the brownish middle of the Mandelbrot set, where points are attracted towards zero for small c.

 

Sphere used to stereographically map complex numbers to colors.
Sphere used to stereographically map complex numbers to colors.

Another property of tanh is that the function has singularities wherever z=\pm \pi n i / 2 c for integer n>0. Since Great Picard’s Theorem, that means that in the vicinity of those points it takes on nearly all other values in the complex plane. So whatever the pattern of the corresponding Julia set is, it will repeat itself near there (including images of the image, and so on).This means that despite most z points being attracted towards zero for c-values inside the unit circle, there will be a complex stitching of undefined points since they will be mapped to infinity, or are preimages of points that get mapped there.

Zoom into the tanh Mandelbrot set, showing chaotic regions with interspersed periodic regions.
Zoom into the tanh Mandelbrot set, showing chaotic regions with interspersed periodic regions.

Zooming into the messy regions shows that they are full of circle-cusp areas where there is a periodic attractor cycle. Between them are the regions where most of the z-plane where the Julia sets live is just pure chaos. Thanks to various classic theorems in the theory of complex iteration we know that if the Julia set has non-empty interior it is the entire complex plane.

Walking around the outside edge of the boring brown circle gives a fun sequence of patterns. At c=1 there are two real fixed points and a straight line border along the imaginary axis. This line of course contains the singularity points where things get sent to infinity, and near them the preimages of all the other singularities on the line: dramatic, but visually uninteresting.

Tanh 'Julia set' for c=1.
Tanh ‘Julia set’ for c=1.

As we move along the circle towards more imaginary c, there is a twisting of the border since each multiplication by c corresponds to a twist: it is now a fractal spiral covered by little spirals. As the twisting gets stronger, the spirals get bigger and wilder (especially when we are very close to the unit circle, where the dynamics has a lot of intermittency: the iterates almost but not quite gets stuck close to certain points, speed away, and then return to make rather elliptic spirals).

Tanh 'Julia set' for c=1.1*exp(0.23*i).
Tanh ‘Julia set’ for c=1.1*exp(0.23*i).
Tanh 'Julia set' for c=1.1*exp(0.5*i).
Tanh ‘Julia set’ for c=1.1*exp(0.5*i).
Tanh 'Julia set' for c=1.1*exp(0.55*i).
Tanh ‘Julia set’ for c=1.1*exp(0.55*i).

When we advance towards a cuspy border in the c-plane we see the spirals unfold into long twisty tentacles just before touching, turning into borders between chains of periodic domains.

Tanh 'Julia set' for c=1.1*exp(0.6*i).
Tanh ‘Julia set’ for c=1.1*exp(0.6*i).

But then the periodic domains start to snake out, filling the plane wildly.

Tanh 'Julia set' for c=1.1*exp(0.6594*i).
Tanh ‘Julia set’ for c=1.1*exp(0.6594*i).

until we get a plane-filling, ergodic Julia set with no discernible structure. For some c-values there are complex tesselations of basins of attraction, and quite often some places are close enough to weakly repelling fixed points to produce small circular false basins of attraction where divergence is slow.

 

Tanh 'Julia set' for c=1.1*exp(0.66*i).
Tanh ‘Julia set’ for c=1.1*exp(0.66*i).

One way of visualizing this is to make a bifurcation diagram like we do for real iteration. Following a curve r e^{i\theta} we plot where iterates end up projected along some line (for example their real or imaginary part, or some combination). To make structure stand out a bit more I decided to color points after where in the whole plane they are, producing a colorful diagram for r=1.1:

bifurk1.1b

(I have some others on Flickr for the imaginary axis, r=1.25 and r=1.5).

Another, more fun way is to turn them into animated gifs. Since Flickr doesn’t handle them well, I have stored them locally instead:

  • Growth of the Mandelbrot set – shows the behaviour of test iterates in the c-plane near the edge. Note the intermittent spirals.
  • Unit circle – following the unit circle.
  • Tanh 1.0 – the same as above, but inverted coordinates: z=\infty is at the center, zero outside the borders.
  • Tanh 1.1 – r=1.1.
  • Tanh 1.5 – r=1.5.
  • Tanh 2.5 – r=2.5.
  • Tanh 5.0 – r=5.0. Rather sedate except for a brief window near \theta=\pi/2.

Note how spirals unfold until they touch each other, forming periodic domains or exploding across the entire plane, making a chaotic full-plane attractor… which often blinks into complex patterns of periodic domains only to return to chaos.

tanhspir125.082