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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Fourier Transform of Pulse Train

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Padmal
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Problems in understanding Lacey's proof of Carleson's theorem.

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Samir
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Liding Yao
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an application of the Poisson summation formula

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How to calcualte the Fourier Transform of a Gaussian pulse with a nonlinear chirp

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user14634
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I evaluated the Fourier series of $\delta(x-nd)$ for integer n between infinity and minus infinity I think this is an expression for an infinite array of delta functions separated by d. When I evaluated the Fourier transform into q space (reciprocal…
Goods
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In the book of Real Analysis by G. B. Folland, there's a short proof of the validity of $\mathcal{F^{-1}}(\hat{f})=f,$ when both $f$ and $\hat{f}$ lie in $L^1(\mathbb{R^n}).$ A first lemma used, since both are in $L^1:$ $$ \int \hat{f}g = \int…
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non-lipschitz fourier transform

As is well known the Fourier transform of a $L^1(\mathbb R)$ function is continuous, bounded and vanishes at infinity. It is also well-known that not every such function is a Fourier transform of some $L^1(\mathbb R)$. Can You provide me with an…
hassan
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prove that if $f(x)$ is real, then $\left | F(s) \right |^2$ is an even function

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