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

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Discrete Fourier Transform interpreted in terms of sampling period

I understand that $$X(k) = \sum_{n=0}^{N-1}x_ne^{-i2\pi \frac{k}{N} n}$$ and $$x(n) = \frac{1}{N}\sum_{k=0}^{N-1}X_k e^{i2\pi \frac{k}{N} n}$$ are the discrete Fourier transform and inverse discrete Fourier transform. How do I…
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If we take the absolute value for sin function, then it becomes even. However, isn't period of this function $\pi$? To find fourier series, 1.Even 2. period $2 \pi$. Can we just treat this function as period $2\pi$?
jessie
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About the orthonormal decomposition of $L^2 (-\pi , \pi) $

For any $f \in L^2 (-\pi, \pi)$, prove that there exists unique orthonormal decomposition with even functions and odd functions : $$ L^2 ( -\pi , \pi) = L^2 _{odd} (-\pi , \pi ) \oplus L^2_{even} (-\pi , \pi).$$
Bamily
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Use trigonometric polynomial to approximate periodic function.

From page 53 of Fourier Analysis by Stein, we have If $f$ is integrable on the circle, then the Fourier series of $f$ is Cesaro summable to $f$ at every point of continuity of $f$. Moreover, if $f$ is continuous on the circle, then the Fourier…
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I am reading a book by Zoran Gajic titled Linear Dynamic Systems and Signals. There were two problems in chapter 3 that I was curious about. The first question asks for the Fourier Transform of a function $x^2(t-5)$, given the Fourier Transform of…
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eigenvalues and eigenfunctions of the laplacian

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Proving Fourier transform of $\int_0^\infty e^{-x}x^{a-1}dx = \Gamma(a)(1+i\omega)^{-a}$

Given $a > 0$, $$f(x) = \begin{cases} e^{-x}x^{a-1}, &\mbox{if } x > 0 \\ 0, & \mbox{if } x \leq 0 \end{cases}$$ Prove the the Fourier transform of $f$, $\hat{f}(\omega)$ is equal to $\Gamma(a)(1+i\omega)^{-a}$. I know the Gamma function is…
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Why isn't the singularity of $1/x$ important while computing its Fourier transform?

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Decay rate of $L^2-$ norms of derivatives of smooth functions

Assume $f\in C^{\infty}(0,1)\times(0,1)$. Is the following true? $$\Bigg(\int_0^1 \Big|\frac{\partial^nf(t,y)}{\partial y^n}\Big|^2dy\Bigg)^{1/2}\leq c^{n+1}n!,\,\,\,\,n=1,2,\cdots,$$ for all $t\in(0,1),$ where $c>0$ is a constant.
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Fourier Transform of simple functions

i got a couple of questions regardion fourier transformations. I'm not that interested Lets take a box/rectangular function as an example. The "Frequency-Spectrum" of that function is would look somewhat like…
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Inverse Fourier Transform by using convolution theorem.

Inverse Fourier Transform of: $$\mathfrak{F}^{-1} \left \{ e^{-\frac{x^2}{2}}{\frac{sinx}{x}} \right \} $$ by using convolution theorem. Since Fourier Transform convolution turns into multiplication - same property holds also for inverse. So, I am…
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best approximation of $f$ in $L^2([0,2\pi])$ as a linear combination of $\sin(kx)$ (with $k∈\{1,2,3,\ldots,10\}$

Let $f$ be a $2\pi$ periodic function. Assume that $f$ is quadratic integrable in the interval $[0,2\pi]$. Consider $f$ as a vector in the Hilbert space $L^2([0,2\pi])$. Give, based on the Fourier coefficients of $f$, the best approximation of $f$…
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