Fourier Transform of a Triangular Voltage Pulse

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Homework Help Overview

This discussion revolves around calculating the Fourier transform of a triangular voltage pulse, a topic situated within the context of a second-year physics course that integrates mathematical tools relevant to quantum mechanics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to calculate the Fourier transform and expresses uncertainty about the characteristics of the resulting function, such as amplitude and width. Some participants suggest factoring the expression to relate it to the sinc function, while others question how to determine the center of the transform based on the cosine term.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the Fourier transform's properties. Some guidance has been offered regarding the relationship to the sinc function, but there is no explicit consensus on the best approach to analyze the transform's attributes.

Contextual Notes

Participants note that the sinc function has not been covered in their coursework, leading to questions about how to analyze the transform without this knowledge. There is also mention of a specific method suggested by the professor regarding finding the general root of the transform.

SeannyBoi71
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Homework Statement


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So this is a physics problem, but this question doesn't really have to do with the "physics" part of it as much as simply calculating the Fourier transform. (This is a second year physics course and our prof is trying to briefly teach us math tools like this in learning quantum mechanics).

Homework Equations



\tilde{g}(\omega) = \frac{1}{\sqrt2\pi} \int g(t) e^{-i \omega t} dt

The Attempt at a Solution


I have done the calculation of g(ω) several times and got an answer

\frac{2}{(\tau \omega ^2 \sqrt2 \pi)} (1 - cos(\omega \tau))

I believe it is right, but since the work to get it is extensive I don't want to type it up unless someone thinks I made an error. My actual concern is that I have a problem sketching the transform. I graphed it on Wolfram so I have a general idea, but I really have no idea how to find the amplitude, width, and whether it should be centred at ω=0 or at a k0 value. Any insight would be greatly appreciated.
 
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SeannyBoi71 said:
\frac{2}{(\tau \omega ^2 \sqrt2 \pi)} (1 - cos(\omega \tau))
Try factoring (1 - cos(\omega \tau)) in terms of sin(ωτ/2) and identify the celebrated 'sinc' function
 
I had to google 'sinc function' to find out what it was... We have not been taught this so surely there is a way to find the attributes of the transform by simply looking at it. Our prof mentioned something about finding the general root of the transform (here it would be whenever the cos term is 1), but I don't know how to relate that to the centre or anything
 
SeannyBoi71 said:
I had to google 'sinc function' to find out what it was... We have not been taught this so surely there is a way to find the attributes of the transform by simply looking at it. Our prof mentioned something about finding the general root of the transform (here it would be whenever the cos term is 1), but I don't know how to relate that to the centre or anything

If you haven't been taught sinc function, then learn it, it's simple enough. Your expression can be written as the square of the sinc function, where behavior of sinc is well understood. I certainly don't know what your prof had in mind, but the sinc function is centered at zero.
 

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