I'm reading section 4.26 in Big Rudin, but I have two questions.
Suppose $f$ is in $L^1(T)$. This means $f$ is the class of all complex, $2\pi$-periodic, and Lebesgue measurable functions on $R^1$ for which the norm $$||f||_p=\{\frac{1}{2\pi}\int_{-\pi}^{\pi} |f(t)|^p dt\}^{1/p}$$ is finite.
For any $f\in L^1(T)$, Fourier coefficients of $f$ is define by the formula $$\hat{f(n)}=\frac{1}{2\pi}\int_{-\pi}^{\pi} f(t)e^{-int} dt$$ where $n$ is an integer.
The Fourier series of $f$ is $$\sum_{-\infty}^{\infty} \hat{f(n)}e^{int},$$
and its partial sums are $$s_N=\sum_{-N}^{N} \hat{f(n)}e^{int}$$ where $N$ is a natural number (include 0).
It is the fact (the Parseval theorem) that for any $f, g \in L^2(T)$, $$ \sum_{n=-\infty}^{\infty} \hat{f(n)}\overline{\hat{g(n)}}=\frac{1}{2\pi}\int_{-\pi}^{\pi} f(t)\overline{g(t)}dt$$ holds.
Next, Rudin says $$\lim_{N \to \infty}||f-s_N||_2=0$$
since a special case of the Parseval theorem yields $${||f-s_N||_2}^2=\sum_{|n|>N}|\hat{f(n)}|^2$$.
I have questions:
1) how did Rudin derive the last identity from the Parseval theorem? Is this equation obtained by putting $f(t)=g(t)=|f-s_N|$? (but I can't reach the answer)
2) Why the last equation gives the limit? I see $||f-s_N||$ decreases if taking the limit, but I don't know what it means to converge to zero.