This is from a test in Fourier analysis:
Define $$ f(\xi)=\int_0^1 \sqrt{x}\rm{sin}(\xi x) \rm{d}x $$ Calculate $$ \int_{-\infty}^\infty |f(x)|^2 \rm{d}x $$
I started with Plancherel's formula, i.e. $$ \int_{-\infty}^\infty |f(x)|^2 \rm{d}x = \frac{1}{2\pi}\int_{-\infty}^\infty |f(\xi)|^2 \rm{d}\xi $$
but what now? Am I supposed to compute the integral of $f(\xi)$ somehow or what should I do?
Added the "idea flow" to the solution.. I don't know maybe it's useful.
Define $\sqrt x$ in $(-1, 1)$ so that it is an odd function. It's fourier transform is
$$\mathcal F (t) = \int_{-1}^1 \sqrt x e^{ixt} dx = \int_{-1}^1 \sqrt x \cos(tx) dx + i \int_{-1}^1 \sqrt x \sin(tx) dx = 2i \int_0^1 \sqrt x \sin(tx) dx = 2if(t)$$
Now $\mathcal F$ and our modified $\sqrt x$ have the same $||\cdot||_2$ norm (plancherel's theorem!) , and you basically want to find $||\mathcal F||_2$.
You should be good to go now! :-)