# 36π/127 conjecture failed

My recent conjecture that the non-differentiable function
$$f(x) = \sum_{i=0}^\infty \frac{sin(2^i x)}{2^i}$$
reaches the maximum at the point $$x_0=36\pi/127$$ appears to be false (thanks to people from sci.math group for pointing it out).
This is demonstrated by the following graph of the differential quotient $$\frac{f(x_0)-f(x_0-h)}h$$, where $$x_0=\frac{36\pi}{127}$$.

Logarithmic (by h) graph of the quotient (f(x0)-f(x0-h))/h. Horizontal axis is h.
Graph of a quotient with the bigger scale makes it more obvious:
Logarithmic (by x) graph of the same quotient (f(x0)-f(x0-h))/h, bigger scale.
As it can be seen from the graphs, at the certain point h between $$10^{-29}$$ and $$10^{-28}$$ the quotient becomes negative, which means that there exists such h, that $$f(x_0+h) > f(x_0)$$. Apparently, the extremal value is h≈1.998e-29, giving $$f(x_0+h) - f(x_0) \approx 3.06\dot10^{-32}$$.
 f(x0)= 1.329833276287310850440418286206506387707650784... f(x0-1.998e-29)= 1.329833276287310850440418286206535446963412182...
An important note about this calculation: the usual IEEE double accuracy (53 bits, about 16 decimal digits) is insufficient, and long doubles must to be used to obtain the result. For the above calculation I used 1000-bit long floating point values having roughly roughly 300 decimal digits. This, I believe, makes the numeric results trustworthy enough.
There is still a possibility that the maximum is reached at some rational multiple of π, but it never be as simple, as 36π/127. I feel a strange mix of frustration and enlightenment regarding this failure, the result seems absolutely counter-intuitive for me. Why $$x_0/\pi$$ is so incredibly close to the rational value? Is it just a fantastic coincidence, or a consequence of a some deeper facts?
This result strongly resembles the "Almost Integer" values in mathematics. it can be re-formulated in the following way:
$$N = \frac{127}\pi \mathrm{argmin} \sum_{i=0}^\infty \frac{sin(2^i x)}{2^i} = 36+\epsilon$$ where $$\left| \epsilon \right| < 10^{-27}$$. I.e. N is an almost integer value.

# Billiard balls and fractals

Virtually any non-stable dynamic system may be used for generating of fractal images. Here is one example, based on ideal planar billiards.
Consider ideal billiard, consisting of round balls, moving and colliding without friction in the rectangular box.
Then let us measure, how much time needs first ball (green one at the picture) to get to the right wall. Below are the images, showing how time until wall collision depends from initial ball velocity. Horizontal and vertical coordinates at the picture plane correspond horizontal and vertical components of the initial ball velocity, color shows, how much time needed ball to reach the right wall. All pictures are 800x600, about 600K

The top-level view of the fractal

Slightly zoomed
High zoom with different color map
Another highly zoomed image

Increased number of balls. Image became more chaotic. Also, different color map chosen.

# The 36π/127 conjecture

Update: the conjecture is apparently wrong.
There is a problem that bothers me for a long time. Consider function f(x), defined in the following way:
$$f(x) = \sum_{n=0}^\infty \frac{sin(2^n x)}{2^n}.$$
Obviously, this sum converges for every real x; and for every x, -2 < f(x) < 2; and f(x) is continuous (due to the uniform convergence of partial sums).
The special thing about f(x) is that it has no derivatives. It may be easily seen from it's graph:
Red graph denotes f(x), gray lines are sin(2nx)/2n.
The red line in the graph is f(x), is obviously a fractal. Using box-counting approach, it's dimension may be approximated as 1.03, though this value tends to decrease, when minimal box size is decreased.
Using numeric methods, I have found that f(x) achieves it's maximal value at point xmax = 0.8905302... (dash line at the graph above) which effectively equals to $$x_0=\frac{36}{127}\pi$$. I am looking for the proof of this fact, but without success.
Following plot may give a key to the solution. It is a logarithmic graph, showing how the function behaves in the close vicinity of the point $$x_0$$.
 Graph of the f(x) in the vicinity of the point x0.
The notable feature of this graph is its periodicity. At other points, f(x) have more complex behavior:

Periodical structure appears only if x is a rational fraction of $$\pi$$. For other values, graph shows chaotic structure: