In mathematics, a Fourier transform (FT) is a mathematical transform that decomposes functions depending on space or time into functions depending on spatial or temporal frequency, such as the expression of a musical chord in terms of the volumes and frequencies of its constituent notes. The term Fourier transform refers to both the frequency domain representation and the mathematical operation that associates the frequency domain representation to a function of space or time.
The Fourier transform of a function of time is a complex-valued function of frequency, whose magnitude (absolute value) represents the amount of that frequency present in the original function, and whose argument is the phase offset of the basic sinusoid in that frequency. The Fourier transform is not limited to functions of time, but the domain of the original function is commonly referred to as the time domain. There is also an inverse Fourier transform that mathematically synthesizes the original function from its frequency domain representation, as proven by the Fourier inversion theorem.
Linear operations performed in one domain (time or frequency) have corresponding operations in the other domain, which are sometimes easier to perform. The operation of differentiation in the time domain corresponds to multiplication by the frequency, so some differential equations are easier to analyze in the frequency domain. Also, convolution in the time domain corresponds to ordinary multiplication in the frequency domain (see Convolution theorem). After performing the desired operations, transformation of the result can be made back to the time domain. Harmonic analysis is the systematic study of the relationship between the frequency and time domains, including the kinds of functions or operations that are "simpler" in one or the other, and has deep connections to many areas of modern mathematics.
Functions that are localized in the time domain have Fourier transforms that are spread out across the frequency domain and vice versa, a phenomenon known as the uncertainty principle. The critical case for this principle is the Gaussian function, of substantial importance in probability theory and statistics as well as in the study of physical phenomena exhibiting normal distribution (e.g., diffusion). The Fourier transform of a Gaussian function is another Gaussian function. Joseph Fourier introduced the transform in his study of heat transfer, where Gaussian functions appear as solutions of the heat equation.
The Fourier transform can be formally defined as an improper Riemann integral, making it an integral transform, although this definition is not suitable for many applications requiring a more sophisticated integration theory. For example, many relatively simple applications use the Dirac delta function, which can be treated formally as if it were a function, but the justification requires a mathematically more sophisticated viewpoint. The Fourier transform can also be generalized to functions of several variables on Euclidean space, sending a function of 3-dimensional 'position space' to a function of 3-dimensional momentum (or a function of space and time to a function of 4-momentum). This idea makes the spatial Fourier transform very natural in the study of waves, as well as in quantum mechanics, where it is important to be able to represent wave solutions as functions of either position or momentum and sometimes both. In general, functions to which Fourier methods are applicable are complex-valued, and possibly vector-valued. Still further generalization is possible to functions on groups, which, besides the original Fourier transform on R or Rn (viewed as groups under addition), notably includes the discrete-time Fourier transform (DTFT, group = Z), the discrete Fourier transform (DFT, group = Z mod N) and the Fourier series or circular Fourier transform (group = S1, the unit circle ≈ closed finite interval with endpoints identified). The latter is routinely employed to handle periodic functions. The fast Fourier transform (FFT) is an algorithm for computing the DFT.
http://ms.mcmaster.ca/courses/20102011/term4/math2zz3/Lecture1.pdfOn pg 10, the example says f(x)=/=0 while R.H.S is zero. It is an equations started from the assumption in pg 9; f(x)=c0f(x)0+c1f(x)1…, then how do we get inequality?
if the system is complete and orthogonal, then...
I am not quite clear on the use of Fourier series to solve the Schrodinger equation.
Can you point me to a source of some simple one dimensional examples?
I'm trying to solve this exercise but I have some problems, because I haven't seen an exercise of this type before.
"f(x)= \pi -x in [0, \pi]
Let's consider the even extension of f(x) in [-\pi, \pi]
and write the Fourier Series using this set ( \frac{1}{\sqrt{2 \pi}}, \frac{1}{\sqrt {\pi}}...
Homework Statement
Sketch the waveform defined below and explain how you would obtain its Fourier series:
f(wt) = 0 for 0 ≤wt ≤pi/2 (w=omega)
f(wt) = Vsin(wt) for pi/2 ≤wt ≤pi
f(wt) = 0 for pi ≤wt ≤3pi/2
f(wt) = Vsin(wt) for 3pi/2 ≤wt ≤2pi
Develop the analysis as far as you are...
Hey guys, long story short. I am completing my Math minor this semester and need to decide on whether Topology or Fourier Analysis. I am an undergraduate physics major and neither one of those classes is required for my B.S. in physics. So what do you guys think, Topology or Fourier Analysis?
Hi Folks,
The Fourier Cosine Transform of cos(x) for 0<x<a and 0 everywhere else is given as
F(\omega)=\displaystyle\frac{1}{\sqrt{2 \pi}}[\frac{\sin a (1-\omega)}{1-\omega}+\frac{\sin a (1+\omega)}{1+\omega}]
I can plot this and we get a continuous amlitude spectrum of F(\omega) against...
when a function doesn't satisfy dirichlet condition, why do we not care and go ahead finding the Fourier transform anyway? What is the use?
Eg: unit impulse, dirac delta function, etc. don't statisfy the dirichlet conditions but its like dirichlet conditions arent really conditions?
Homework Statement
[/B]
f(x)=\left\{\begin{array}{cc}0,&\mbox{ if }
0< x < 2\\1, & \mbox{ if } 2<x<4\end{array}\right.
Show that the Cosine Fourier Series of f(x) for the range [0,4] is given by:
A + B\sum^{\infty}_{n=0}\frac{(-1)^n}{(2m+1)}cos(\frac{(2m +1) \pi x}{2})
Homework Equations...
Homework Statement
Noting that J_0(k) is an even function of k, use the result of part (a) to
obtain the Fourier transform of the Bessel function J_0(x).
Homework Equations
In (a) I am asked to show that the Fourier transform of
f(x)=\dfrac{1}{\sqrt{1-x^{2}}}
is...
Homework Statement
The question is to get Fourier sine series of e^-x =f(x) on 0<x<1
Homework Equations
Bn = 2/L ∫ (e^-x) * sin(nπx/L) over the limits 1 to 0, where L = 1
f(x) = summation of Bn*sin(nπx/L)
The Attempt at a Solution
So I integrated ∫ by part integration
so I took u =...
Homework Statement
So the question is how does
4/π*(sin(πx))+4/3π *(sin(3πx))+4/5π *(sin(5πx)) = 1
for values of 0<x<1
Homework Equations
No relevant equation needed just don't understand which values of x to take.
The Attempt at a Solution
I am not sure which value of x to start with, it...
Why is the summation for the discrete Fourier series from 0 to N-1 (where N is the fundamental period of the signal) wheras it goes from minus infiniti to infiniti for continuous Fourier series...Thank you
Hi
To properly understand introductory quantum mechanics, I want to understand what the Fourier transform actually gives me mathematically. What book do you recommend? I found one book, but it doesn't get to Fourier transformations until after seven long chapters. Is that what I have to expect...
So I have been away from education for a little while now and I'm going through some refresher stuff - in particular I have been playing around with FFTs.
If i take (with MATLAB notation):
time = 0:0.01:10
y = fft(sin(2*pi*f*time))
with f = 5
then the maximum amplitude of the fft output is...
Homework Statement
This comes up in the context of Poisson's equation
Solve for ##\mathbf{x} \in \mathbb{R}^n ## $$ \nabla^2 G(\mathbf{x}) = \delta(\mathbf{x})$$
Homework Equations
$$\int_0^\pi \sin\theta e^{ikr \cos\theta}\mathop{dk} = \int_{-1}^1 e^{ikr \cos\theta}\mathop{d\cos \theta
}$$...
Hello everyone,
I'm in need for the best books that you know out there for PDE (Partial Differential Equations) and everything related to Fourier (series, transform, etc.).
Any help would be much appreciated.
Thank you and happy holidays!
Homework Statement
this is something i noticed doing homework rather than homework itself. I plot fft output from different frequency signals, i am not sure why power changes with increasing frequency?
Homework Equations
if i take (with MATLAB notation):
time = 0:0.01:10
y =...
Homework Statement
I am having trouble understanding this:
I have a Dirac Delta function
$$ \delta (t_1-t_2) $$
but I want to prove that in the frequency domain (Fourier Space), it is:
$$\delta(\omega_1+\omega_2) $$
Would anyone have any ideas how to go about solving this problem?
I know...
Hi, I've been reading a paper on renormalisation theory as applied to a simple one-particle Coulombic system with a short-range potential.
In the process of renormalisation, the authors introduce an ultraviolet cutoff into the Coulomb potential through its Fourier transform:
## \frac{1}{r}...
Hello everyone,
I know that the integral of an odd function over a symmetric interval is 0, but there's something that's bothering my mind about it.
Consider, for example, the following isosceles trapezoidal wave in the interval [0,L]:
When expressed in Fourier series, the coefficient...
I'm recently new to the field of 2D Fourier Transform Infrared Spectroscopy and am learning its applications. I would like to know its applications in biology. Specifically, is there anything in the 400 nm to 1000 nm range that is important in protein structure, protein dynamics or biology in...
Alright guys.
First off, this is my first post (happy to be here!) and I'm hoping this is the correct section of the forum. I'm an engineering student, currently working towards finishing my master's thesis.
Short introduction. I am trying to simulate an ocean wave environment, as a...
I'm asked to transform y(t) = x(t)*x(t) (where * is the convolution product) and x(t)= sinc(t)cos(2π10t) ( sinc(t)= sin(πt)/(πt) ).The attempt at a solution
Clearly everything is simple if you know X(f), because y(t)=InverseFourier{ X(f)2 }. The problem is that I can't find X(f). By the way...
Hi, friends! In order to find an orthogonal basis of eigenvectors of the Fourier transform operator ##F : L_2(\mathbb{R})\to L_2(\mathbb{R}),f\mapsto\lim_{N\to\infty}\int_{[-N,N]}f(x)e^{-i\lambda x}d\mu_x## for Euclidean separable space ##L_2(\mathbb{R})##, so that ##F## would be represented by...
Homework Statement
Evaluate following series:
\sum_{n=1}^\infty \frac{1}{(4n^2-9)^2}
by finding the Fourier series for the 2\pi-periodic function
f(x) =
\begin{cases}
sin(3x/2) & 0<x<\pi \\
0 & otherwise
\end{cases}
Homework Equations
a_n = \frac{1}{\pi}\int_{-\pi}^{\pi}...
I am carrying out FFT analysis to compare two waves. One looks very much like a sine wave the other has an extra dip occurring at half the frequency of the main wave. I have been thinking around how I might expect this to show up in the FFT analysis. At first i was expecting to see a smaller...
Homework Statement
Find the following Fourier series in trigonometric form.
Homework Equations
$$y(t)=a_0+\sum\limits_{n=1}^{\infty} a_n cos(n\omega_{0}t)+b_n sin(n\omega_{0}t)$$
The Attempt at a Solution
The graph above is represented by the function:
$$
x(t) = \left\{
\begin{array}{ll}...
Homework Statement
A damped harmonic oscillator is driven by a force of the form f(t)=h(t) t^2 Exp(-t), where h(t) is a Heaviside step function. The Oscillator satisfies the equation x''+2x'+4x=f(t). Use pencil-and-paper methods involving Fourier transforms and inverse transforms to find the...
Homework Statement
Using a theorem (state which theorem you are using and give the formula), Calculate the Fourier Transform of
1. rect(x)triangle(x)
2.cos(pi*x)sinc(x)
3.rect(x)exp(-pi*x^2)
4.sinc(x)sin(pi*x)
5. exp(-pi*x^2)cos(pi*x)
Homework Equations
not sure what theorem to use for the...
Homework Statement
Homework Equations
The Attempt at a Solution
I don't really understand why my solution is wrong as I think I have substituted everything in correctly..
Is it okay if anyone can help me take a look at my solution? Thank you. :)
My solution: (Only bn)
My...
Homework Statement
Find the inverse Fourier transform of
X(ejw = 1/(1-ae-jw)2
using the convolution theorem.
Homework EquationsThe Attempt at a Solution
I tried finding the partial fraction coefficients but without success.
(NOTE: Maybe this post belongs in the Number Theory Forum? Apologies if it is wrongly located!)
I am reading Julian Havil's book, "The Irrationals: The Story of the Numbers You Can't Count On"
In Chapter 4: Irrationals, Old and New, Havil gives a proof of the irrationality of e which was...
Hi, friends! Let ##f:[a,b]\to\mathbb{C}## be an http://librarum.org/book/10022/173 periodic function and let its derivative be Lebesgue square-integrable ##f'\in L^2[a,b]##. I have read a proof (p. 413 here) by Kolmogorov and Fomin of the fact that its Fourier series uniformly converges to a...
Hello, everybody. I am currently working on deriving solutions for Stokes flows. I encounter a multidimensional inverse Fourier transform. I already known the Fourier transform of the pressure field:
\tilde{p}=-\frac{i}{{{k}^{2}}}\mathbf{F}\centerdot \mathbf{k}
where i is the imaginary unit...
Homework Statement
Hi, so I am doing some past exam papers and there was this question;
Homework EquationsThe Attempt at a Solution
a0 and an both are equal to zero, this leaves only bn.
Since you can only use the sine series for an odd function, and cos(t) is even, does this mean i have to...
If you take the Fourier series of a function $f(x)$ where $0 < x < \pi$, then would $a_{0}$, $a_{n}$, and $b_{n}$ be defined as,
$a_{0} = \displaystyle\frac{1}{\pi}\int_{0}^{\pi}f(x)dx$
$a_{n} = \displaystyle\frac{2}{\pi}\int_{0}^{\pi}f(x)\cos(nx)dx$
$b_{n} =...
Hello,
I hope somebody can help me with this.
1. Homework Statement
I am supposed to show that if there is a function \phi(x,t) which is real, satisfies a linear wave equation and which satisfies \phi(x,0)=0 for x<0 then the Fourier Transform \tilde{\phi}(k) of \phi(x,0) is in the lower...
Can anyone point me to some material on applying the Fourier transform to the case of an analytic function of one complex variable?
I've tried to generalize it myself, but I want to see if I'm overlooking some important things. I've started by writing the analytic function with
u + iv where u...
Homework Statement
I was working on a problem where I had been given a differential equation to be solved using separation of variables. Two coordinates: a time coordinate and a single spatial coordinate (1-D problem).
Homework Equations
The domain for the spatial part was [0, L].
Given...
Homework Statement
Find Fourier series of f(x) = Acos(\pix/L)
I know how to do this, I just don't know the value of L. If it's equal to \lambda/2, then I know the solution. But the question does not specify the value of L. L is just the length of the entire wave that I'm working with, right? If...
Hi everybody! I'm studying the Fourier integral operators but I can't resolve a pass. I'm considering the following operator:
$$Au(x)=\frac{1}{{(2\pi h)}^{n'}}\int_{\mathbb{R}_y^m\times\mathbb{R}_\theta^{n'}} e^{i\Psi(x,y,\theta)/h}a(x,y,\theta,h)u(y)\, dy\, d\theta$$ where $$Au\in C^0...
we have a wavefunction \psi (x) the question asks for \psi (p) and says to use this to calculate the expectation value of momentum. The problem is the expectation value of momentum is integrated over dx so after transforming how do you get the integral to be over dp?
thanks for any help with...
Ok so this isn't a homework question per se, but I'm currently writing a report on Fourier Analysis but a bit stuck as to what the results can actually help with. I realized that I don't grasp how a Fourier Transform can be used.
In the experiment we recorded the signal created by a remote...
Suppose we have some function f(x) with period L. My book states that if it is even around the point x=L/4, it satisfies f(L/4-x)=-f(x-L/4), whilst if it is odd it satisfies f(L/4-x)=f(x-L/4). Then we define s=x-L/4 so we have for the function to be odd or even about L/4 that f(s)=±f(-s)...
Homework Statement
The problem is finding the Fourier series of f(t) = e^(-t) from [0,2] where T=2 and without using complex solution.
[/B]Homework Equations
f(t) = a0/2 + ∑ (anCos(nωt) +bnsin(nωt)
NOT using f(t) = ∑dne^(inωt)The Attempt at a Solution
I tried once but got completely wrong...
Homework Statement
Define ##f : [−π, π) → \mathbb R ## by
##f(x)## = ##−1## if ##− π ≤ x < 0##, ##1## if ##0 ≤ x < π.##
Show that the Fourier series of f is given by
##\frac{4}{π} \sum_{n=0}^\infty \frac{1}{(2k+1)} . sin(2k+1)x##Homework Equations
The Fourier series for ##f## on the interval...
Hi there,
I am reading a material on the application of Fourier transformation in physics. One application is to transform the position-dependent function to k-dependent function, i.e.## F(k) = FFT[f(x)]##
We know that the in physics, the wavenumber could be written in momentum as...
Hi Folks,
I need to evaluate the following function f(t)=A[1+B \cos(\omega_1 t+ \phi)] \cos(\omega_2 t+ \phi) to find f(\omega) using the Fourier transform.
Ie, the Fourier transform I use is
f(\omega)=\displaystyle \frac{1}{\sqrt {2 \pi}} \int^{\infty}_{-\infty} f(t) (\cos \omega t+ j \sin...
Hi, I need help with some basic Fourier transform properties stuff - its fairly simple though I think I am doing something wrong.
So we know from the shifting property
if h(x) has the Fourier transform H(f)
then h(x-a) has the Fourier transform H(f)ei*2*π*f*a
so I have the function
cos(2πf0x...