I have a a coin infinitely thin, rotating along the diameter. How to derive the formula for it's moment of inertia passing through the diameter.
I was suggested to use the surface density and infinitely small part of the surface area, equidistant from the axis of rotation (marked as $dS$ on the picture).

I've already figured out that:
$$I~=~\int r^2dm~=~\int \rho r^2 dS. $$
And now I'm stuck.
Any help would be much appreciated. Greg
edit:
My coin is infinitely thin, so it's two-dimensional object (only $X$ any $Y$ axis). So let's assume that my rotating axis is equal to Y axis. So I have to integrate from $R$ to $-R$ on the $X$ axis. And every $dS$ will have different surface area. But I know, that total area is $S=\pi r^2$. From Pythagorean theorem I know, that $ r^2 + h^2 = R^2 $. And my integrate is $$I ~=~ \int\limits_{-R}^{R} 2\rho r^2 \sqrt {R^2 - r^2} dr $$
But now I'm confused how to solve that - every time I get different solution than in Wolfram Alpha calculator
Ok, I've solved that - final answer is $ I = \frac {1}{4}MR^2 $