Integral of sinc function using Fourier series

  • #1
psie
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Homework Statement
Show that the Fourier coefficients of $$u(x)=\begin{cases} \frac{\sin x}{x} & 0<|x|\leq\pi, \\ 1 & x=0.\end{cases}$$ are $$c_n=\frac{1}{2\pi}\int_{(n-1)\pi}^{(n+1)\pi}\frac{\sin x}{x}dx.$$ Use this to evaluate ##\int_0^\infty \frac{\sin x} x dx##.
Relevant Equations
I'm not sure.
Showing that the (complex) Fourier coefficients of ##u(x)## are as specified is a simple exercise, which I've managed to do, but how do I then go about evaluating ##\int_0^\infty \frac{\sin x} x dx##? The coefficients do not have an explicit formula, right? Note, the Fourier transform has not been introduced yet. I thought this has something to do with Riemann-Lebesgue's lemma or even Parseval's identity, but probably I'm mistaken.
 
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  • #2
By evenness of [itex]\sin x/x[/itex], [tex]\begin{split}
\int_0^\infty \frac{\sin x}x\,dx &= \frac12 \int_{-\infty}^{\infty} \frac{\sin x}x\,dx \end{split}.[/tex] To evaluate the right hand side, one can either split the real line into intervals of width [itex]2\pi[/itex] centered at even multiples of [itex]\pi[/itex] or into intervals of width [itex]2\pi[/itex] centered at odd multiplies of [itex]\pi[/itex]. The results must be the same*, so [tex]
\begin{split}\int_{-\infty}^\infty \frac{\sin x}x\,dx &= \frac12 \left(\sum_{n=-\infty}^\infty \int_{((2n)-1)\pi}^{((2n)+1)\pi} \frac{\sin x}{x}\,dx
+ \sum_{n=-\infty}^\infty \int_{((2n+1)-1)\pi}^{((2n+1)+1)\pi} \frac{\sin x}{x}\,dx \right) \end{split}[/tex]

*Assuming the integral exists, which I don't believe this method establishes.
 
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  • #3
pasmith said:
*Assuming the integral exists, which I don't believe this method establishes.
Which integral do you mean?

If I understand you right, this is your argument: ##\sum_{n\in\mathbb Z} c_n## is just the function evaluated at ##0##, so we have $$1=\sum_{n\in\mathbb Z} c_{2n}+\sum_{n\in\mathbb Z}c_{2n+1}=\frac{2}{2\pi}\int_{-\infty}^\infty \frac{\sin x} x dx.$$ And by evenness, we conclude that ##\int_0^\infty \frac{\sin x} xdx=\frac{\pi}{2}##.
 
  • #4
I assume you mean $$\int_{-\infty}^\infty \frac{\sin x} x dx.$$ In my computation above it seems like we require ##\sum_{n\in\mathbb Z} c_n## to converge absolutely, so that one can rearrange the series and sum the even terms first and then the odd one's, or vice versa.
 
  • #5
I think I take back the requirement of absolute convergence. If ##\sum_{k\geq} a_k## converges, we can always write $$\sum_{k\geq 1}a_k = \sum_{k\geq 1}(a_{2k}+a_{2k-1}),$$ but not $$\sum_{k\geq 1}a_k = \sum_{k\geq 1}a_{2k}+\sum_{k\geq 1}a_{2k-1}.$$ Here, however, we can write the series in the latter form, since, assuming that ##\int_{-\infty}^\infty \frac{\sin x} x dx## converges, we have that ##\sum_{n\in\mathbb Z} c_{2n}## and ##\sum_{n\in\mathbb Z}c_{2n+1}## both converge.
 
  • #6
pasmith said:
By evenness of [itex]\sin x/x[/itex], [tex]\begin{split}
\int_0^\infty \frac{\sin x}x\,dx &= \frac12 \int_{-\infty}^{\infty} \frac{\sin x}x\,dx \end{split}.[/tex] To evaluate the right hand side, one can either split the real line into intervals of width [itex]2\pi[/itex] centered at even multiples of [itex]\pi[/itex] or into intervals of width [itex]2\pi[/itex] centered at odd multiplies of [itex]\pi[/itex]. The results must be the same*, so [tex]
\begin{split}\int_{-\infty}^\infty \frac{\sin x}x\,dx &= \frac12 \left(\sum_{n=-\infty}^\infty \int_{((2n)-1)\pi}^{((2n)+1)\pi} \frac{\sin x}{x}\,dx
+ \sum_{n=-\infty}^\infty \int_{((2n+1)-1)\pi}^{((2n+1)+1)\pi} \frac{\sin x}{x}\,dx \right) \end{split}[/tex]

*Assuming the integral exists, which I don't believe this method establishes.
I'm confused. Could you clarify what you are suggesting on how to evaluate ##\int_{-\infty}^\infty \frac{\sin x} x dx##? I don't see how this is possible unless we have absolute convergence of ##\sum_{n\in\mathbb Z} c_n##.
 
  • #7
It is easier to justify if one starts from [tex]\begin{split}
\sum_{n=-N}^N c_n &= \sum_{n=-N}^N \frac{1}{2\pi} \int_{(n-1)\pi}^{(n+1)\pi} \frac{\sin x}x\,dx \\
&= \frac{1}{2\pi}\int_{-(N+1)\pi}^{-N\pi} \frac{\sin x}{x}\,dx + \frac{1}{\pi}\int_{-N\pi}^{N\pi} \frac{\sin x}x\,dx + \frac{1}{2\pi}\int_{N\pi}^{(N+1)\pi} \frac{\sin x}x\,dx \\
&= \frac{2}{\pi} \int_0^{N\pi} \frac{\sin x}x\,dx + \frac1\pi \int_{N\pi}^{(N+1)\pi} \frac{\sin x}x\,dx\end{split}[/tex] so that [tex]
\left| \sum_{n=-N}^N c_n - \frac2\pi \int_0^{N\pi} \frac{\sin x}x\,dx \right| = \left|\frac 1\pi \int_{N\pi}^{(N+1)\pi} \frac{\sin x}{x}\,dx \right| \leq \frac 1\pi \int_{N\pi}^{(N+1)\pi} \frac 1x\,dx = \frac1\pi \log\left(1 + \frac 1N \right).[/tex]
 
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FAQ: Integral of sinc function using Fourier series

What is the sinc function?

The sinc function, denoted as sinc(x), is defined as sinc(x) = sin(x)/x for x ≠ 0 and sinc(0) = 1. It is a mathematical function that arises frequently in signal processing and Fourier analysis.

Why is the integral of the sinc function important in Fourier series?

The integral of the sinc function is important in Fourier series because the sinc function is the Fourier transform of the rectangular function. This relationship is fundamental in signal processing, where the sinc function is used to reconstruct continuous signals from their samples.

How can the Fourier series be used to compute the integral of the sinc function?

The Fourier series can be used to compute the integral of the sinc function by expressing the sinc function as a sum of sinusoidal components. By integrating these components individually and summing the results, one can derive the integral of the sinc function over a specified interval.

What are the challenges in integrating the sinc function using Fourier series?

One of the main challenges in integrating the sinc function using Fourier series is the convergence of the series. The sinc function has an infinite number of oscillations, which can make it difficult to obtain a closed-form solution for its integral. Careful analysis and sometimes numerical methods are required to handle these oscillations.

Can the integral of the sinc function be expressed in a closed form?

Yes, the integral of the sinc function over the entire real line can be expressed in a closed form. The result is known as the Dirichlet integral, which states that the integral of sinc(x) from negative infinity to positive infinity is π. However, for finite intervals, the integral may not always have a simple closed-form expression.

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