Questions tagged [fourier-analysis]

Fourier analysis, also known as spectral analysis, encompasses all sorts of Fourier expansions, including Fourier series, Fourier transform and the discrete Fourier transform (and relatives). The non-commutative analog is (representation-theory).

Fourier analysis is the study of how general functions can be decomposed into trigonometric or exponential functions with definite frequencies. There are two types of Fourier expansions:

  • Fourier series: If a (reasonably well-behaved) function is periodic, then it can be written as a discrete sum of trigonometric or exponential functions with specific frequencies.
  • Fourier transform: A general function that isn’t necessarily periodic (but that is still reasonably well-behaved) can be written as a continuous integral of trigonometric or exponential functions with a continuum of possible frequencies.

The reason why Fourier analysis is so important is that many (although certainly not all) of the differential equations that govern physical systems are linear, which implies that the sum of two solutions is again a solution. Therefore, since Fourier analysis tells us that any function can be written in terms of sinusoidal functions, we can limit our attention to these functions when solving the differential equations. And then we can build up any other function from these special ones. This is a very helpful strategy, because it is invariably easier to deal with sinusoidal functions than general ones.

Fourier series

Consider a function $f(x)$ that is periodic on the interval $0 ≤ x ≤ L$, then Fourier’s theorem states that $f(x)$ can be written as $$f(x)={a_0}+\sum_{n=1}^{\infty}\left[a_n \cos\left(\frac{2n\pi x}{L}\right)+b_n \sin \left(\frac{2n\pi x}{L}\right)\right]$$ where the constant coefficients $a_n$ and $b_n$ are called the Fourier coefficients of $f$ and is given by $$a_0=\frac{1}{L}\int_0^L f(x)\mathrm{d}x$$ $$a_n=\frac{2}{L}\int_0^L f(x)\cos\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$ $$b_n=\frac{2}{L}\int_0^L f(x)\sin\left(\frac{2\pi nx }{L}\right)\mathrm{d}x$$

Reference:

http://www.people.fas.harvard.edu/~djmorin/waves/Fourier.pdf

https://en.wikipedia.org/wiki/Fourier_analysis

http://mathworld.wolfram.com/FourierSeries.html

Fourier Transform:

For this part find the following link

https://math.stackexchange.com/tags/fourier-transform/info

10420 questions
3
votes
1 answer

Is a positive-definite function which is also in $C_0(\mathbb{R}^n)$ necessarily the Fourier transform of a positive $L^1$-function?

I have got the following question. From Bochner's theorem we know that a continuous, positive-definite function is the Fourier transform of a positive, bounded measure on $\mathbb{R}^n$. It is also known that the Fourier transform of a function $f…
Jan M.
  • 125
3
votes
0 answers

The Fourier transform of $ \begin{cases} 1 & |x|<1\\ 0 & else \end{cases} $ where $x \in \mathbb R^3$ is an elementary function?

Consider the following function in $\mathbb{R}^3$ $$ \begin{cases} 1 & |x|<1\\ 0 & \text{else} \end{cases}$$ How can we calculate its Fourier transform (again, in $\mathbb{R}^3$). I tried to use spherical coordinates in order to calculate $$…
FreeZe
  • 3,735
3
votes
1 answer

Inequality for an integrable real valued function with a compactly supported Fourier transform

Let $f$ be an integrable function on $\mathbb{R}$ where $\operatorname{support}(\widehat{f}) \subseteq [-\gamma, \gamma]$ for some $ 0 < \gamma < 1$ Prove that $\lvert f(x) - f(0)\rvert \leq c \gamma \lvert x\rvert \sup\limits_{ y \in…
jessica
  • 31
3
votes
1 answer

Intuitive way to understand the square wave spectrum?

What is a intuitive way to understand that a transform of a square wave can result into something like this?
user8005
  • 379
3
votes
1 answer

Need help with Fourier transform problem

I'm trying to calculate the Fourier transform of the unit step function, $$\mathcal{F}[u(t)] \ = \int_{-\infty}^{\infty}u(t)e^{-i\omega t}dt \ = \int_{0}^{\infty}e^{-i\omega t} dt. \tag{1}$$ This simplifies to, $$U(\omega) = (i\omega)^{-1},\ (\omega…
3
votes
0 answers

Fourier coefficient of the dilation $f_m := f(mt)$

Let $f \in L^1(\mathbb{T})$ and $m \in \mathbb{N}$. Furthermore, define the dilation $f_m$ by $f_m(t) := f(mt)$ for any $t \in \mathbb{T}$. I would like to show that $$ \widehat{f_m}(n) = \begin{cases} \hat{f}(n/m) \ \ \ \ \ \ \text{if} \ m \…
Vicky
  • 891
3
votes
1 answer

Uniqueness of Fourier representation

I started to read about Fourier analysis. I was just reading about uniqueness of the Fourier representation. Apparently if the Fourier series $\sum\limits_{n\in \mathbb{Z}}c_n e^{2\pi i n x}$ converges uniformly to $f(x)$ then the values of $c_n$…
roi_saumon
  • 4,196
3
votes
1 answer

Fourier Transform is onto $L^2(\mathbb{R})$

In Introduction to Fourier Analysis on Euclidean Spaces, the authors explore the $L^2$ extension of the Fourier transform and argue that it is onto $L^2(\mathbb{R})$ but I can't follow their reasoning. Here is their proof from page 17: Theorem 2.3.…
3
votes
2 answers

Proof of Fourier Transform

Where F is the fourier transform, how can you show that $$\mathcal F(x\cdot f(x)) = −i \frac{d\mathcal F}{dw}.$$ I understand that you are meant to apply the inverse transform to the left hand side, but I just can not seem to get it to work. Many…
R.M
  • 311
3
votes
1 answer

$2\pi$-periodic $L^2$ functions on $R^1$ approximated by its Fourier series

I'm reading section 4.26 in Big Rudin, but I have two questions. Suppose $f$ is in $L^1(T)$. This means $f$ is the class of all complex, $2\pi$-periodic, and Lebesgue measurable functions on $R^1$ for which the norm…
aaaa
  • 143
3
votes
2 answers

Help to find complex Fourier series coefficient of this periodic function

I'm having big trouble finding the complex Fourier series coefficient of the following periodic function $$\frac{a-b\cos\varphi}{\sqrt{a^2+b^2-2ab\cos\varphi}}$$ Mathematica is unable to compute it!!
3
votes
0 answers

Fourier transform in spherical space

Recall that in 3 dimensions, the Fourier transforms are defined as following: $$ \tilde{f}(\textbf{k})= \frac{1}{(2\pi)^{3/2}} \int_{0}^{\infty}f(\textbf{x}) e^{-i\textbf{k}\cdot\textbf{x}} d^3x$$ $$f(\textbf{x}) = \frac{1}{(2\pi)^{3/2}}…
3
votes
1 answer

Fourier Analysis an Introduction chap3 Problem 2

(c) Prove that any polynomial of degree n that is orthogonal to $1,x,x^{2},...,x^{n-1}$ is a constant multiple of $L_{n}.$ $$L_{n}=\frac{d^{n}}{dx^{n}}(x^{2}-1)^{n}$$ Two elements $X$ are $Y$orthogonal if $(X,Y)=0$ for $(X,Y)$ is defined…
John He
  • 539
3
votes
1 answer

Getting the amplitudes back from fft without using ifft

I have a wave that is a sum of sines and cosines: $$x = A\sin(\omega t + \phi_1) + B \cos(2\omega t + \phi_2) + C\sin(2\omega t + \phi_3) + D\cos(2\omega t + \phi_4).$$ Now I use fft on $x$ and get the magnitude with abs(fft(x)). How do I get $A$,…
3
votes
1 answer

Solving the heat equation using Fourier series

I'm interested in using the Fourier transform to solve the heat equation. I've been poring over this wikipedia article: http://en.wikipedia.org/wiki/Heat_equation#Solving_the_heat_equation_using_Fourier_series trying to understand it but every time…
user21154
  • 345