Sine Fourier series and coefficient of Fourier series

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SUMMARY

The discussion focuses on deriving the sine Fourier series for the function \( f(x) = x(\pi - x) \) over the interval \( 0 \leq x \leq \pi \). Participants confirm that the Fourier coefficients are given by \( a_n = \frac{1}{\pi} \int_0^{\pi} x(\pi - x) \cos(nx) \, dx \) and \( b_n = \frac{2}{\pi} \frac{1 - (-1)^n}{n^3} \). The conversation also explores the implications of these coefficients, including the convergence of specific series involving sine functions and their relationships to known constants. Additionally, the discussion touches on the properties of odd piecewise continuous functions and their Fourier series representation.

PREREQUISITES
  • Understanding of Fourier series, particularly sine Fourier series.
  • Knowledge of integration techniques for piecewise functions.
  • Familiarity with convergence of series and properties of sine functions.
  • Basic concepts of periodic functions and their characteristics.
NEXT STEPS
  • Study the derivation of Fourier coefficients for different types of functions.
  • Learn about convergence tests for Fourier series, particularly for sine series.
  • Explore the implications of odd and even functions in Fourier analysis.
  • Investigate the application of Fourier series in solving differential equations.
USEFUL FOR

Mathematicians, physics students, and engineers interested in Fourier analysis, particularly those working with periodic functions and series convergence. This discussion is also beneficial for anyone looking to deepen their understanding of sine Fourier series and their applications.

Markov2
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1) Find the sine Fourier series of $f(x)=x(\pi-x),\,0\le x\le\pi$ and show that $\displaystyle\sum_{k\ge1}\frac{(-1)^k}{(2k-1)^3},\,\sum_{k\ge1}\frac1{(2k-1)^6}$ and $\displaystyle\sum_{k\ge1}\frac{\sin\big((2k-1)\sqrt5\pi\big)}{(2k-1)^3}$ and to show that $\displaystyle\sum_{k\ge0}\frac{\sin(2n-1)x}{(2n-1)^3}>0$ for all $x\in(0,\pi).$

2) Let $f$ be an odd piecewise continuous function of period $4L$ and which is even with respect $x=L.$ Show that the Fourier series of $f$ is $\displaystyle\sum_{n\ge1}b_{2n-1}\sin\frac{(2n-1)\pi}{2L}x,$ where $b_{2n-1}=\displaystyle\frac2L\int_0^L f(x)\sin\frac{(2n-1)\pi}{2L}x\,dx.$

Attempts:

1) I don't know how to find the Fourier series here, how to work with a non-symmetric interval?

2) No ideas here, how to start?
 
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Markov said:
1) Find the sine Fourierseries of $f(x)=x(\pi-x),\,0\le x\le\pi$...

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

$\displaystyle a_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} x\ (\pi-x) \cos nx\ dx = \left\{\begin{array}{cl}\frac{\pi^{2}}{6},&n=0\\ \frac{(-1)^{n}}{\pi\ n^{2}},&n > 0\end{array}\right.$

$\displaystyle b_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} x\ (\pi-x) \sin nx\ dx = \frac{2}{\pi}\ \frac{1 - (-1)^{n}}{n^{3}}$

Kind regards

$\chi$ $\sigma$
 
Last edited:
Okay, makes sense! Could you help me with second part?
 
First of all I need to correct my previous post because the values of the $a_{n}$ aren't correct (Headbang)... Here the Fourier coefficients for...

$f(x)=\begin{cases} x\ (\pi-x) &\text{if}\ 0< x<\pi\\ 0 &\text{if}\ -\pi<x\le 0\end{cases}$


$\displaystyle a_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} x\ (\pi-x) \cos nx\ dx = \left\{\begin{array}{cl}\frac{\pi^{2}}{6},&n=0\\ \frac{(-1)^{n}}{n^{2}},&n > 0\end{array}\right.$

$\displaystyle b_{n}= \frac{1}{\pi}\ \int_{0}^{\pi} x\ (\pi-x) \sin nx\ dx = \frac{2}{\pi}\ \frac{1 - (-1)^{n}}{n^{3}}$

Very sorry!...

Kind regards

$\chi$ $\sigma$
 
The results obtained in the last post permits us to write...

$\displaystyle f(x)= \frac{\pi^{2}}{12} - (\cos x - \frac{1}{4}\ \cos 2x +\frac{1}{9}\ \cos 3x - \frac{1}{16}\ \cos 4x +...) + \frac{4}{\pi}\ (\sin x + \frac{1}{27}\ \sin 3x + \frac{1}{125}\ \sin 5x +...)$ (1)

... where for $0 \le x < \pi $ is $f(x)=x\ (\pi-x)$. Setting in (2) $x=0$ we obtain...

$\displaystyle \frac{\pi^{2}}{12}= 1 - \frac{1}{4} + \frac{1}{9} - \frac{1}{16}+...$ (2)

... and setting in (2) $x=\frac{\pi}{2}$ we obtain...

$\displaystyle \frac{\pi^{3}}{32} = 1 - \frac{1}{27} + \frac{1}{125} -...$ (3)

Other values of $0 \le x < \pi $ can be inserted in (2) obtaining more interesting results and the task is left to the reader...

Kind regards

$\chi$ $\sigma$

 
The task is greatly more simple using the 'double identity', easy obtainable from the Fourier expansion just described...

$\displaystyle \frac{\pi^{2}}{12} - (\cos x - \frac{1}{4}\ \cos 2x +\frac{1}{9}\ \cos 3x - \frac{1}{16}\ \cos 4x +...) = \frac{4}{\pi}\ (\sin x + \frac{1}{27}\ \sin 3x + \frac{1}{125}\ \sin 5x +...)= \frac{x\ (\pi-x)}{2}$ (1)

... where for $0 \le x \le \pi $. For example setting in (1) $x=\frac{\pi}{4}$ You obtain...

$\displaystyle 1 + \frac{1}{27} - \frac{1}{125} - \frac{1}{343} +... = \pi^{3}\ \frac{3}{64\ \sqrt{2}}= 1.02772258593...$ (2)

Kind regards

$\chi$ $\sigma$

 
In the last post we have seen that the'identity'...

$\displaystyle \frac{4}{\pi}\ (\sin x +\frac{1}{27}\ \sin 3x + \frac{1}{125}\ \sin 5x +...)= \frac{x\ (\pi-x)}{2}$ (1)

... is true for $0 \le x \le \pi$ and in that interval the 'infinite sum' is greater or equal to 0. A simple question: whatabout $-\pi \le x \le 0$?... the answer is easy: in that case change the sign of second term of (1)...

In the starting post it was requested the value of $\displaystyle\sum_{n=0}^{\infty} \frac{(-1)^{n}}{(2n+1)^{3}}\ \sin (2n+1) x$ for $x=\pi\ \sqrt{5}$... because is $\displaystyle \pi \sqrt{5}= \pi (\sqrt{5}-2)\ \text{mod}\ 2 \pi$ is...

$\displaystyle \sum_{n=0}^{\infty} \frac{(-1)^{n}}{(2n+1)^{3}}\ \sin (2n+1)\ \pi \sqrt{5} = \frac{11 - 5 \sqrt{5}}{8}\ \pi^{3} = -.6989585560358...$ (2)

Kind regards

$\chi$ $\sigma$

 
Thanks a lot! That helped me a lot! Could you help me with second problem please?
 
For the second problem is essential for me to understand better that...

Markov said:
... let $f$ be an odd piecewise continuous function of period $4L$ and which is even with respect $x=L$...

... what does it mean that?... may be that is even in the two half periods and odd in the full period?...

Kind regards

$\chi$ $\sigma$
 
  • #10
Sorry for the delay, well, I wouldn't know really what exactly that means. :(
 

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