I tried to do this in polar coordinates setting the perimeter to $L_0$ and using 'by parts' to break this integral down.
$$\int_{0}^{2\pi}rd{\theta} = L_0$$ and $$A=\frac{1}{2}\int_{0}^{2\pi}r^2d{\theta}$$.
Integration by parts leads to
$$\frac{1}{2}(L_0r(0) - \int_{0}^{2\pi}\int rd\theta\frac{dr}{d\theta}d{\theta})=\frac{1}{2}L_0r(0)-\frac{1}{4}\int_{0}^{2\pi}r^2d{\theta}$$
So $A = \frac{1}{2}L_0r(0) - \frac{1}{2}A$ and $A = \frac{1}{3}L_0r(0)$. where $r(0)$ is the radius at an arbitrary point.
I was hoping to find an equation for the area that I could use $r(\theta)$ to maximise (by intuition), instead I got quite possibly the most ridiculous answer. Namely, that the area of all 2d shapes is $\frac{1}{3}L_0r(0)$. Why is this?