A homogeneous cylinder with radius a and mass m rolls in a hollow cylinder with radius R. Determine the kinetic energy of the cylinder as function of $\dot{\theta}$.
Alright, I found this problem inside an old textbook of mine. Strangely enough there was no drawing to this, so I was kind of baffled about where $\theta$ actually is.
I tried drawing this and while drawing I noticed two angles that might fit the description.

Although while imagining the smalle cylinder rolling inside I thought it should be the angle I coincidentally also denoted as $\theta$, right?
So I tried approaching this problem with this angle, but I just don't know how to start there. A couple of weeks ago we talked about rotational energy and I was thinking that maybe it only has rotational energy since there is no translational energy if I'm not mistaken? So, $E=I\omega ^2$? But I don't know how to get $\omega=\dot{\theta}$.
So the hard part is working out the moment of inertia of the small cyclinder. We are told it's uniform so it has inertia around it's centre of $\frac{1}{4}ma^2$ So now we use the parallel axes theorem and it's inertia around the centre of the hollow cylinder is $(\frac{1}{4}a^2+(R-a)^2)m$. So now we use the formula for inertia and get $ E=\frac{1}{2}I\theta^2=\frac{1}{2}(\frac{1}{4}a^2+(R-a)^2)^\theta^2 $