I was wondering how we derive these formulas, and why we have a separate formula for $a_0$? All I know from advanced engineering mathematics text book are following formulas but where do they come from?
$$a_0 = \frac{1}{2L} \int_{-L}^{L} f(x) dx,~~~~a_n = \frac{1}{L} \int_{-L}^{L} f(x) \cos{\frac{n\pi x}{L}}dx,~~~~b_n = \frac{1}{L} \int_{-L}^{L} f(x) \sin{\frac{n\pi x}{L}} dx$$
I found the proof somewhere on net!
for some function with some properties we have: $$ \int _0 ^Tf(x)dx = \int_\alpha ^{\alpha + T}f(x)dx $$
and now we have(suppose that $L = \pi$): $$ f(x) = a_0 + \sum _{n=1}^{\infty}(a_n\cos(nx) + b_n\sin(nx)) $$
If we Integrate from $[-\pi, \pi]$ from above we have: $$ \int_{-\pi}^{\pi}f(x)dx = \int_{-\pi}^{\pi}a_0 + \sum _{n=1}^{\infty}\int_{-\pi}^{\pi}(a_n\cos(nx) + b_n\sin(nx)) $$ the sum goes to zero and finally we have: $$ \int_{-\pi}^{\pi}f(x)dx = 2\pi a_0 $$
for $a_n$ we multiply the general form with $\cos(nx)$ for $b_n$, $\sin(nx)$ comes to play, this method is due to Euler and is named Euler formulas, And also fourier him self did it this way!