Question 2 of 7: Fourier Series and a Classical Identity
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Notes on this paper
EGBC National Examination — 04-BS-5 Advanced Mathematics, December 2015. Closed-book, 3-hour exam;
candidates were permitted one 8.5"x11" aid sheet (both sides) and an approved calculator. The exam
instructs that any five questions constitute a complete paper (first five answers in the answer book are marked); every question is solved below as a full study resource.
Given. $f(x)$ is $2\pi$-periodic, piecewise linear on $(-\pi,0]$ and constant on $(0,\pi]$, as
defined above.
Find. (A) The full Fourier series $a_0/2+\sum(a_n\cos nx+b_n\sin nx)$; (B) use it at $x=0$
to derive the Basel-type identity for $\pi^2/8$.
Approach. Compute $a_0$, $a_n$, $b_n$ from the Euler–Fourier formulas by splitting each
integral at $x=0$; then evaluate the series at the continuity point $x=0$ (both branches agree there, $f(0)=\pi$)
to extract the numerical identity.
Mean value $a_0$.
$$a_0=\frac{1}{\pi}\int_{-\pi}^{0}(x+\pi)\,dx+\frac{1}{\pi}\int_{0}^{\pi}\pi\,dx
= \frac{1}{\pi}\left(\frac{\pi^{2}}{2}\right)+\pi = \frac{3\pi}{2}\ \Rightarrow\ \frac{a_0}{2}=\frac{3\pi}{4}.$$
Cosine coefficients $a_n$. On $(0,\pi]$, $\int_0^\pi \pi\cos(nx)\,dx = \pi\sin(n\pi)/n = 0$.
On $(-\pi,0]$, substituting $u=x+\pi$ (so $u:0\to\pi$) and using $\cos(nx)=\cos(nu-n\pi)=(-1)^n\cos(nu)$:
$$\int_{-\pi}^{0}(x+\pi)\cos(nx)\,dx = (-1)^n\int_0^\pi u\cos(nu)\,du = \frac{1-(-1)^n}{n^{2}}.$$
Hence $a_n=\dfrac{1-(-1)^n}{\pi n^{2}}$, i.e.
$$\boxed{a_n = 0\ (n\text{ even}), \qquad a_n=\frac{2}{\pi n^{2}}\ (n\text{ odd}).}$$
Sine coefficients $b_n$. The same substitution on the sine integral gives, after combining both branches,
$$\boxed{b_n = \frac{(-1)^{n+1}}{n}, \qquad n=1,2,3,\dots}$$
Assemble the series (part A).
$$f(x) = \frac{3\pi}{4} + \sum_{\substack{n=1\\ n\ \text{odd}}}^{\infty}\frac{2}{\pi n^{2}}\cos(nx)
+ \sum_{n=1}^{\infty}\frac{(-1)^{n+1}}{n}\sin(nx).$$
Part B — evaluate at $x=0$. Both branches of $f$ agree at $x=0$: the left branch gives
$f(0^-)=0+\pi=\pi$ and the right branch's limit is also $\pi$, so $f$ is continuous there and the Fourier series
converges to $f(0)=\pi$. Setting $x=0$ in the series (every $\sin$ term vanishes):
$$\pi = \frac{3\pi}{4} + \sum_{\substack{n=1\\ n\ \text{odd}}}^{\infty}\frac{2}{\pi n^{2}}
\ \Rightarrow\ \sum_{\substack{n=1\\ n\ \text{odd}}}^{\infty}\frac{1}{n^{2}} = \left(\pi-\frac{3\pi}{4}\right)\frac{\pi}{2}
= \frac{\pi}{4}\cdot\frac{\pi}{2}.$$
Re-indexing the odd integers as $n=2k-1$ gives the required identity:
$$\boxed{\frac{\pi^{2}}{8} = \sum_{k=1}^{\infty}\frac{1}{(2k-1)^{2}}}$$