The Golden Self-Contracting Angles
The golden ratio is \[ \phi = \frac{1+\sqrt{5}}{2}. \] It is the unique positive solution to the equation \(x^2-x-1=0\), and its reciprocal \(1/\phi\) is the unique positive solution to \({x^2+x-1=0}\). Two useful properties of \(\phi\) are that \[ \begin{align} \frac{1}{\phi} &= \phi-1 \\ \frac{1}{\phi^2} &= 2-\phi \end{align} \] See the Wikipedia article for more information.Below is the graph of the self-contacting scaling factor as a function of $\theta$, along with the horizontal line at \(1/\phi \approx 0.61803\). We see that there are exactly four intersections. We claim that these occur at $\theta$ = 60°, 108°, 120°, and 144°.
Case: $\theta = 60^\circ$
When $0 \lt \theta \lt 90^\circ$, the self-contacting scaling factor $r$ is the unique solution [Proof] to the equation \[\sum_{k=0}^{N-1} r^{k+2}\cos(k\theta) = \frac{1}{2}\] where $N$ is the smallest integer such that $N\theta \ge 90^\circ$. If $\theta$ = 60°, then $N$ = 2, and the equation for $r$ is \[ \frac{1}{2} = r^2 + r^3\cos(60^\circ) = r^2 + \frac{r^3}{2} \\ \\ \Rightarrow 0 = r^3 + 2r^2 - 1 = (r^2 + r - 1)(r+1) \] Therefore $r$ satisfies \(r^2+r-1=0\), and hence \(r = 1/\phi\).Case: $\theta = 108^\circ$
For $90^\circ \lt \theta \lt 135^\circ$, the self-contacting factor $r$ satisfies the equation [Proof] \[ (*) \quad 2\cos(2\theta)r^2 + 2\cos(\theta)r + 1 = 0 \]
If $\theta$ = 108°, then
\[
\begin{align}
\cos(108^\circ) &= \frac{1-\sqrt{5}}{4} = -\frac{1}{2\phi} = -\frac{1}{2}(\phi-1) \\ \\
\cos(216^\circ) &= 2\cos^2(108^\circ) - 1 = \frac{1}{2\phi^2}-1 = -\frac{\phi}{2}
\end{align}
\]
Substituting these into (*) gives
\[
2\cos(2\theta)r^2 + 2\cos(\theta)r + 1 = -\phi r^2 - (\phi-1)r + 1 = -(\phi r - 1)(r+1) = 0
\]
Therefore \(r_{sc} = 1/\phi\) is the solution when $\theta$ = 108°.
Casse: $\theta = 120^\circ$
We can still use (*) with $\theta$ = 120°. This gives \[ \begin{align} 2\cos(2\theta)r^2 + 2\cos(\theta)r + 1 &= 2\cos(240^\circ)r^2 + 2\cos(120^\circ)r + 1 \\ \\ &= -r^2 - r + 1 = r^2+r-1 \end{align} \] and so \(r_{sc} = 1/\phi\) is the solution when $\theta$ = 120°.Case: $\theta = 144^\circ$
For $135^\circ \lt \theta \lt 180^\circ$, the self-contacting value is [Proof] \[r_{sc} = -\frac{1}{2\cos(\theta)}\]
Therefore when $\theta$ = 144°, we have
\[
r_{sc} = -\frac{1}{2\cos(144^\circ)} = -\frac{1}{-2\cos(36^\circ)} = \frac{1}{2\left(\frac{1+\sqrt{5}}{4}\right)} = \frac{2}{1+\sqrt{5}} = \frac{1}{\phi}.
\]
