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
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Find occurrences of sequences in sound wave

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Convergence of convolution

I have a vector $x = (..., x_{-1}, x_0, x_1, ...)$ and a vector $w = (..., 0, 0, 1, 1, .. , 1, 1, 0, 0, ..)$ (with $2M + 1$ components equals to 1) such that $y = x \cdot w = (0, 0, .., x_{-M},x_{-M + 1}, .., x_{M-1}, x_M, 0, 0, ..) $ (product…
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How do I interpret continuous time fourier transform plot?

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Solve integral equation using convolution

I'm trying to solve an integral equation by identify the convolution and then transforming, but I'm getting to a really confusing expression, where I'm not sure how to continue: $$ \int_{-\infty}^{\infty}f(t-y)e^{-|y|}dy=e^{-t^2/2} $$ Any ideas?…
Curtain
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question about 1D & 2D Fourier transformation

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Problem about Fourier transform being integrable

I am currently reading a paper and the author makes the following claim: If $f \in L^1(\mathbb{R})$ is a continuous, even, and nonnegative function such that $\hat{f}(\alpha) \leq 0$ for $|\alpha| \geq 1$, then $\hat{f} \in L^1(\mathbb{R})$. He…
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why locally integrable g can't exist with schwartz function

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Drawing conclusion on function differentiability based on the fourier coefficient bound

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distribution 0 in fourier transform clarification

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The meaning of the angle of Fourier coefficients.

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Decay in Fourier coefficients

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Show that $\sum_{n=1}^{\infty}(-1)^n\frac{\sin(nx)}{n} = \frac{-x}{2}$ for $-\pi < x < \pi$.

Show that $\sum_{n=1}^{\infty}(-1)^n\frac{\sin(nx)}{n} = \frac{-x}{2}$ for $-\pi < x < \pi$. I rewrote to $\sum_{n=1}^{\infty}\frac{\sin(n(x+\pi))}{n}$, but then I'm stuck.
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Fourier transform of $(x^2+b^2)^{-1}$

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Introduction to Fourier Analysis Question, Chapter 6 exercise 7

I am currently enrolled in a Fourier analysis class and I am having such trouble with this problem question description Would anyone be able to help me understand what to do?
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If $f \in L^2(\mathbb{R}^n)$ and $T \in S^*(\mathbb{R}^n)$. Then: there exists $F \in L^2(\mathbb{R}^n)$ such that $\hat{T}_f=T_F$

I' asked to show the following statement: Let $f \in L^2(\mathbb{R}^n)$ and $T \in S^*(\mathbb{R}^n)$. Then there exists $F \in L^2(\mathbb{R}^n)$ such that $\hat{T}_f=T_F$ (where the hat denotes the Fourier transform). My first problem: I suppose…