Three cool facts about rotations of the circle

I was playing around with GeoGebra and made this applet about one of the simplest, but most intersting dynamical systems: the rigid rotation of a circle. Let me tell you a little about this fascinating subject.

Let S^1 denote a circle. For simplicity, let’s think of it as a circle with circumference 1. Let a be any real number. Define a function f_a:S^1\to S^1 as follows: if x is a point on S^1, then f_a(x) is obtained by rotating x counterclockwise a units.

There are a few other equivalent ways of thinking of this. You may want to think of S^1 as the interval [0,1] with the points 0 and 1 glued together. Or you may want to think of it as \mathbb{R}/\mathbb{Z}; that is, take the real number line and wrap it up like a slinky so that all points that differ by an integer are glued together. In these cases we can write our function as f_a(x)=x+a\text{ (mod }1).

We may view this function as a dynamical system. Given a point x, we obtain the orbit of x by plugging it into f_a repeatedly: x, f_a(x), f_a(f_a(x)), f_a(f_a(f_a(x))),\ldots. As usual we will use the familiar notation that n compositions of the function, (f_a\circ\cdots\circ f_a)(x), is denoted f^n_a(x). However, in this case f^n_a(x)=f_{na}(x). In other words, rotating n times by a is the same as rotating once by na.

This is not a chaotic dynamical system—far from it. Points do not get mixed up at all, this is a rigid rotation of the circle.

Cool fact #1.

The behavior of the orbits differ depending on whether a is or is not rational. If a is rational, then every point is periodic. The period of each point is the same; it is the value of the denominator of a (assuming a is expressed as a reduced fraction). On the other hand, if a is irrational, then not only are the orbits not periodic, they are dense in the circle. By this we mean that the orbit “fills up” the entire circle (or more precisely, given any point of the circle, there is a subsequence of the orbit that converges to this point).

Theorem. If a is rational, then every point is periodic. If a is irrational, then every point has a dense orbit.

Cool fact #2.

The previous theorem states that the orbit of any point under an irrational rotation is dense. However we can say more than this. It turns out that if we look at the limiting behavior of an orbit, we see that it fills up the circle uniformly (technically, we say that the function is uniquely ergodic).

Theorem. Let a be irrational and I be an arc in S^1. Let m(n) be the cardinality of I\cap\{0,f_a(0),f_a^2(0),\ldots,f_a^{n-1}(0)\}. Then \text{length}(I)= \displaystyle\lim_{n\to\infty}\frac{m(n)}{n}.

In other words, the fraction of the time that the orbit spends in I is precisely the length of the interval I.

Cool fact #3.

Consider a finite orbit segment: \{0,f_a(0),f_a^2(0),\ldots,f_a^{n-1}(0)\}. These n points divide the circle into arcs various lengths. It turns out that for a fixed n, the lengths come in only one, two, or three sizes. Moreover, if there are three lengths, then one is the sum of the other two!

Three Gap Theorem (The Steinhaus Conjecture). The points \{0,f_a(0),f_a^2(0),\ldots,f_a^{n-1}(0)\} divide S^1 into arcs of one, two, or three lengths. If there are three lengths, then one is the sum of the other two.

To see  the three gap theorem in action, view this GeoGebra applet.

Picture 1

There is a lot more one can say about rigid rotations of the circle; they have interesting connections to dynamical systems, topology, the study of continued fractions, number theory, symbolic dynamics, etc. Go explore!



  1. watchmath says:

    Cool! I think the fact that f_a(x) is dense can be prove by using Pigeon Hole Principle.

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