Set of points reachable by the tip of a swinging sticks kinetic energy structure This is an interesting problem that I thought of myself but I'm racking my brain on it. I recently saw this kinetic energy knick knack in a scene in Iron Man 2:
http://www.youtube.com/watch?v=uBxUoxn46A0
And it got me thinking, it looks like either tip of the shorter rod can reach all points within the maximum radius of device.
The axis of either rod is off center, so for simplicity I decided to first simplify the problem by modeling it as having both rods centered. So the radius of the device is $r_1 + r_2$. So I decided to first model the space of points reachable by the tip of the shorter rod as a function of a vector in $\mathbb{R}^2$, consisting of $\theta_1$, the angle of the longer rod, and $\theta_2$, the angle of the shorter rod.
Where I'm getting lost is how to transform this angle vector to its position in coordinate space. How would you describe this mapping? And how would you express the space of all points reachable by the tip of the shorter rod, as the domain encompasses all of $\mathbb{R}^2$?

One way to see the reach is to notice that if the configuration $\theta = (\theta_1,\theta_2)$ reaches some spot $x \in \mathbb{R}^2$, and $y$ is a spot obtained by rotating $x$ by $\alpha \in \mathbb{R}$, then the configuration $\theta+(\alpha, \alpha)$ will reach $y$. So, we only need to see what the minimum and maximum radius can be.
For a particular configuration, the radius squared is 
\begin{eqnarray}
(r_1 \cos \theta_1 + r_2 \cos \theta_2)^2 + (r_1 \sin \theta_1 + r_2 \sin \theta_2)^2 &=& r_1^2+r_2^2+ 2r_1r_2 ( \cos \theta_1 \cos \theta_2 + \sin \theta_1 \sin \theta_2)\\
& = & r_1^2+r_2^2+ 2r_1r_2 \cos(\theta_1-\theta_2)
\end{eqnarray}
Hence the radius lies in $[|r_1-r_2|,|r_1+r_2|]$.
