MHB Compute Fourier Series of f(x)=sin(x) & Parseval's Identity

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The discussion focuses on computing the Fourier series for the piecewise function f(x) defined as sin(x) when sin(x) is non-negative and 0 otherwise. Participants discuss the method for finding the Fourier coefficients a_n and b_n, with one contributor providing the explicit formulas for these coefficients. Additionally, the conversation shifts to using Parseval's identity to demonstrate that the sum of the series involving odd integers equals π²/8. The challenge of integrating the function squared is also addressed, particularly regarding the behavior of f(x) in different intervals. The thread concludes with clarifications on the function's definition and its implications for the Fourier series computation.
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1) Compute Fourier series of $f(x)=\left\{\begin{array}{cl}\sin x,&\sin x\ge0,\\0,&\sin x<0.\end{array}\right.$

2) Consider the $2\pi-$periodic function $f(x)=\left\{\begin{array}{cl}1,&\text{ if }\phantom{-}0\le x<\pi,\\0,&\text{ if }-\pi\le x<0.\end{array}\right.$ Use Parseval's identity to prove that $\displaystyle\sum_{n\ge1}\frac1{(2n-1)^2}=\frac{\pi^2}8.$

Attempts:

1) How can I get the bounds to compute the Fourier series?

2) I think this is straightforward, I just need t compute $a_n$ and $b_n$ by writing for example $a_n=\displaystyle\frac1\pi\int_{-\pi}^{\pi}f(x)\cos (nx)\,dx=\frac{1}{\pi }\left( {\int_{ - \pi }^0 {f(x)\cos (nx)\,dx} + \int_0^\pi {f(x)\sin (nx)\,dx} } \right),$ and the same for $b_n,$ the rest is using $\displaystyle\frac{{a_0^2}}{2} + \sum\limits_{n = 1}^\infty {\left( {a_n^2 + b_n^2} \right)} = \frac{1}{\pi }\int_{ - \pi }^\pi {f{{(x)}^2}\,dx} ,$ but I have a problem here, when calculating the integral of the last formula, I'd need to split it up into two integrals but the fact that $f(x)=1$ for $0\le x<\pi$ doesn't imply that $f(x)^2=1,$ doesn't?
 
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Markov said:
1) Compute Fourier series of $f(x)=\left\{\begin{array}{cl}\sin x,&\sin x\ge0,\\0,&\sin x<0.\end{array}\right.$

If f(x) is $2 \pi$ periodic You have...

$\displaystyle a_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} \sin x\ \cos nx\ dx = \frac{1}{\pi} \frac{-1+(-1)^{n+1}}{n^{2}-1}$

$\displaystyle b_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} \sin x\ \sin nx\ dx = \left\{\begin{array}{cl}\frac{1}{2},&n=1\\0,&n \ne 1\end{array}\right.$

Kind regards

$\chi$ $\sigma$
 
Last edited:
Okay but why $0\le x<\pi$ ?
 
Markov said:
Okay but why $0\le x<\pi$ ?

For $- \pi< x<0$ [or, that is the same, for $-1< \sin x<0$...] is $f(x)=0$...

Kind regards

$\chi$ $\sigma$
 
There are probably loads of proofs of this online, but I do not want to cheat. Here is my attempt: Convexity says that $$f(\lambda a + (1-\lambda)b) \leq \lambda f(a) + (1-\lambda) f(b)$$ $$f(b + \lambda(a-b)) \leq f(b) + \lambda (f(a) - f(b))$$ We know from the intermediate value theorem that there exists a ##c \in (b,a)## such that $$\frac{f(a) - f(b)}{a-b} = f'(c).$$ Hence $$f(b + \lambda(a-b)) \leq f(b) + \lambda (a - b) f'(c))$$ $$\frac{f(b + \lambda(a-b)) - f(b)}{\lambda(a-b)}...

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