If $f$ is a Riemann integrable function on $[0,2\pi]$ such that $f(x)=0$ whenever $f$ is continuous at $x$, then: \begin{equation} \|f\|=\left(\frac{1}{2\pi}\int_0^{2\pi}|f(x)|^2dx \right)^{1/2}=0 \end{equation}
How do I go about proving this without any measure theory? I've thought about using the fact that the Cesaro mean of the Fourier series converges to 0 at all points of continuity but it leads to nowhere.