Solving a Problem With Fourier Transforms: Heaviside Unit Step Function

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Homework Help Overview

The discussion revolves around the application of Fourier transforms to the Heaviside unit step function, specifically focusing on the function f(x) defined as f(x)=H(x)-H(x-l). Participants are exploring the Fourier integral representation of this function and its implications for a related integral calculation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants are attempting to derive the Fourier integral representation for the odd extension of the function f(x) and are questioning the relationship between g(x) and f(x). There is also discussion about the assumptions regarding the variable l, particularly its sign and implications for the function's behavior.

Discussion Status

The discussion is ongoing, with participants providing insights and clarifications regarding the definitions and relationships of the functions involved. Some guidance has been offered regarding the assumptions about l, but there is no explicit consensus on the approach to the integral or the behavior of the functions.

Contextual Notes

There are mentions of potential issues with the rendering of LaTeX in the forum, which may affect the clarity of mathematical expressions shared by participants. Additionally, the definition of the Heaviside function and its implications for the problem setup are under consideration.

Telemachus
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Hi there. I'm starting with the Fourier transforms, and I'm having some trouble with my first exercise on this topic.
The problem says: Given f(x)=H(x)-H(x-l) (H(x) is the Heaviside unit step function).
a) Consider the odd extension for f and find its Fourier integral representation.
b) Using the previous incise calculate the value for \int_0^{\infty}\frac{1-cos (\omega l)}{\omega}\sin (\omega l) d\omega

Well, for a) I think I should get the Fourier transfor for the sign function, I don't know if this is right, but anyway I've defined the function like this:
attachment.php?attachmentid=36336&stc=1&d=1307746243.png


Then the Fourier integral representation:
g(x)=\displaystyle\frac{1}{2\pi}\displaystyle\int_{-\infty}^{\infty}\displaystyle\int_{-\infty}^{\infty}g(x)e^{-i \omega x}dx e^{i \omega x}d\omega

But g(x) is odd, then:

attachment.php?attachmentid=36337&stc=1&d=1307746243.png


And the thing is that the integral for the cosine diverges as I see it, but I'm probably doing something wrong.

Help please :)

PD, I don't know why latex isn't working in some cases, so I've attached some images.
 

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Can you tell us how your g(x) is related to the f(x) in the problem statement?

Also, is there any assumption regarding whether l is positive, negative, or zero?

If l is positive, then f(x) should be 1 for 0 < x < l and 0 elsewhere. (Change < to \leq as appropriate, depending on how you defined the Heaviside function.)

P.S. Your Latex looks fine, but be aware that it doesn't seem to render correctly in your own browser after you first post it. If you refresh the page, it should fix itself.
 
Hi jbunni. Thanks for posting.

Can you tell us how your g(x) is related to the f(x) in the problem statement?
Yes, g(x) is the odd extension for f(x). Here you have a graph of both, I take l=2, but l is arbitrary (I think that when I find the Fourier Integral I must be doing something like l->infinity, so I think I should get the sign function):
attachment.php?attachmentid=36341&stc=1&d=1307753650.png


You're right about that it must be 1 at x=0. But it doesn't make any difference I think.

About latex, I've realized that sometimes I have to refresh to see the "pictures" instead of the code, but today it just didn't work, and for some commands (the brackets for example, to define a trunked function) it just doesn't work for me, I've tried to refresh, but it didn't work, so then I've uploaded the pictures.
 

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The odd function can be also defined as g(x)=H(x)-H(x-l)-H(-x)+H(-x-l)
 

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