Understanding Roel Snieder's Fourier Transform Conventions

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Homework Help Overview

The discussion revolves around a problem from Roel Snieder's book regarding the Fourier transform and the response of a linear time-invariant system to an input signal. Participants are exploring the relationship between the system's impulse response and the output generated by a specific input signal.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to clarify the definitions of the system's response and input signal, with some suggesting a reformulation of the problem for clarity. There is also exploration of the convolution theorem and its implications for the output of the system.

Discussion Status

The discussion is ongoing, with participants providing insights and questioning the conventions used in the Fourier transform equations. There is recognition of differing conventions in the literature, and some participants express uncertainty about the implications of these differences on their understanding of the problem.

Contextual Notes

Participants note that the problem assumes a linear time-invariant system, and there is mention of potential discrepancies in the scale factors used in the Fourier transform equations, which are causing confusion. The original poster has been grappling with the problem for an extended period, indicating a challenging aspect of the material.

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Homework Statement



Show that for a fixed value of [itex]\omega[/itex] that [itex]G(\omega)e^{-i\omega t}[/itex] is the response of the system to the input signal [itex]e^{-i\omega t}[/itex].

(From Roel Snieder's book 'A Guided Tour of Mathematical Methods for the Physical Sciences', pg 233 (Section 15.7, Problem e))

2. Homework Equations (I think)

The Fourier transform pair:

[itex]f(t)=\int^{\infty}_{-\infty}F(\omega)e^{-i\omega t}d\omega[/itex]

[itex]F(\omega)=\frac{1}{2\pi}\int^{\infty}_{-\infty}f(t)e^{i\omega t}dt[/itex]

Convolution relations:

[itex]o(t)=\int^{\infty}_{-\infty}g(t-\tau)i(\tau)d\tau[/itex]

[itex]O(\omega)=2\pi G(\omega)I(\omega)[/itex]

The Attempt at a Solution



I'm not really sure I understand the question. I am assuming that the 'response of the system' is [itex]g(t)[/itex] and that 'input signal' is [itex]i(t)[/itex]. I could well be wrong on that.

So I am reading the question as saying: show that for the case [itex]i(t)=e^{-i\omega t}[/itex] ...

[itex]g(t)=G(\omega)e^{-i\omega t}[/itex].

I have tried playing around with the symbols but I have not managed to get thing to click, which makes me suspect that I am misunderstanding the question. I have been sitting on this problem for weeks and have managed to progress through the book no problem, but not getting this question is bugging me.

Any help would be greatly appreciated.
 
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g(t) is the impulse response of the system, as you pointed out in the convolution relations :biggrin:
It would be clearer I think if we rewrite the question like this: show that for a system of impulse response g(t), the response to the input [itex]e^{-i\omega _0t}[/itex] is [itex]G(\omega _0)e^{-i\omega _0t}[/itex].
 
Hi hikaru, thanks for quick reply.

Just to be clear, by

...the response to the input [itex]e^{-i\omega _0t}[/itex] is [itex]G(\omega _0)e^{-i\omega _0t}[/itex]

Do you mean the output, [itex]o(t)[/itex] is [itex]G(\omega _0)e^{-i\omega _0t}[/itex]?
 
Yup.
 
Oh I forgot this: the system should be linear time-invariant. Otherwise, it would be absurd to mention G(w) without any clarification.
 
OK so let me see ...

Rewrite the convolution theorem such that:

[itex]o(t)=\int^{\infty}_{-\infty}g(\tau)i(t-\tau)d\tau[/itex]

Let [itex]i(t-\tau)=e^{-i\omega (t-\tau)}[/itex], (in compliance with the original question,) such that:

[itex]o(t)=\int^{\infty}_{-\infty}g(\tau)e^{-i\omega (t-\tau)}d\tau[/itex]

Consider the Fourier transform of [itex]g(\tau)[/itex]:

[itex]G(\omega)=\frac{1}{2\pi}\int^{\infty}_{-\infty}g(\tau)e^{i\omega \tau}d\tau[/itex]

And plug this into above to get:

[itex]o(t)=2\pi G(\omega)e^{-i\omega t}[/itex].

I'm off by a factor of [itex]2\pi[/itex], where did I go wrong?
 
You should check the relations you wrote in your post 1 section 2 :smile: They're wrong.
 
hikaru1221 said:
You should check the relations you wrote in your post 1 section 2 :smile: They're wrong.

Really, I just checked them in the textbook and they're not wrong (unless the book's wrong).

I was thinking that the [itex]2\pi[/itex] dropped out from my choice of scale factor in my Fourier transform, and so it is arbitrary...?
 
  • #10
OK so if I changed that scale factors around for my Fourier transforms it would work, and I'm kind of happy with that because it means I understand it (up to a fair level). But something is still out of place, making me feel uneasy and uncertain about whether I really do understand it.

Why would the book be wrong? The book sticks to the convention and it works in all the other examples perfectly... so what is it about this particular problem that makes this issue stick out?

And what are the reasons for not having the scale factors this was around? I was under the impression that it didn't matter, as long as the product of the scale factors is equal to [itex]1/2\pi[/itex]. If I can get these issues straight in my head I will be happy. :smile:
 
  • #11
The book is not so wrong; it just uses a different set of conventions (but not very practically applicable to physics/ science though, in my opinion). Under those conventions, the factor of 2*pi should be there. However, the question follows the popular convention, and so, the factor is not there in the question. Perhaps the author messes up himself :biggrin: just kidding :wink:
 
  • #12
HaHa :biggrin:

Thanks

Maybe I will email the author and see what he has to say :wink:
 
  • #13
I think you should also ask him about the motivation that he decided on using his rather "own" set of conventions for the F-transform pair. To me, his way is quite counter-intuitive.
 

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