Dirac Delta: Finite Height in Fourier Analysis

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Discussion Overview

The discussion revolves around the Dirac delta function and its representation in Fourier analysis, particularly addressing the apparent contradiction between its theoretical definition as an infinite height impulse and its practical depiction with finite height in various contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question the relationship between the Dirac delta function and the sinc function, suggesting that the Dirac delta is not simply a sinc function with infinite height.
  • One participant emphasizes that the Dirac delta function is defined to be zero everywhere except at a specific point, where it is infinite, and that its integral equals one.
  • Another participant notes that in Fourier analysis, the Dirac delta function is represented with a finite height (e.g., 1/2) and questions the reasoning behind this representation.
  • A participant suggests that the arrow notation used to represent impulses in Fourier analysis does not imply a finite height but rather indicates the magnitude of the coefficient associated with the Dirac delta function.
  • One participant recalls that the Fourier Transform of a Dirac delta function results in a flat response across all frequencies, leading to the conclusion that summing infinite frequencies can yield a high amplitude at a point.
  • There are suggestions to explore related discussions in other sub-forums for a deeper theoretical understanding of the Dirac delta function.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the Dirac delta function and its representation in Fourier analysis. No consensus is reached regarding the implications of its finite height representation.

Contextual Notes

Participants highlight the complexity of defining the Dirac delta function, noting its classification as a "distribution" or "generalized function" in mathematics, which may lead to misunderstandings in practical applications.

frenzal_dude
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Hi,
if the definition of a dirac delta (impulse) function is just a sinc function with an infinite height and 0 width, why is it that they are shown and used in Fourier analysis as having a finite height?

for example g(t) = cos(2*PI*f0*t) has two impulses of height = 1/2 at f=+/-f0
 
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I don't know that Dirac Delta function has anything to do with sync function.

The definition of one dimension ( say x ) Dirac Delta function \delta(x-a) is equal zero everywhere except equal to infinity at x=a and

\int_{-\infty}^{\infty}\delta(x-a)dx=\int_{a^-}^{a^+}\delta(x-a)dx=1

Sync function is just sync(x)=\frac{\sin x}{x} and equal to 1 when x=0.
 
ok maybe the sinc was a bad example,
but still, if it is equal to infinity at x=a, why do they represent the impulse as having a finite height of 1/2 in Fourier analysis?
 
i would suggest going to the Wikipedia site for the Dirac delta function.

for a strict mathematician, the definition is not simple. in fact, mathematicians would say that the Dirac delta is not even a function. they like to call it a "distribution" or a "generalized function". i am not all that sure of what they mean, but one thing i remember from my college daze was, in the EE class \delta(t) is a function that is zero everywhere except t=0 and its integral is 1. but in a Real Analysis class (where you learn the difference between Riemann and Lebesgue integration) any function that is zero "almost everywhere" has an integral that is zero. so there's some kinda disconnect there.

for practical purposes, treat the dirac impulse as one of those "nascent" delta functions (the spikes with unit area that get thinner and thinner), but be careful when you find yourself talking about it with your math prof.
 
frenzal_dude said:
ok maybe the sinc was a bad example,
but still, if it is equal to infinity at x=a, why do they represent the impulse as having a finite height of 1/2 in Fourier analysis?

You may have seen something like an arrow. This arrow notation would not mean the impulse has a finite height equal to 1/2. The arrow may have a specific height to indicate the magnitude of the coefficient of the [delayed] Dirac delta it represents.
 
Last edited:
frenzal_dude said:
ok maybe the sinc was a bad example,
but still, if it is equal to infinity at x=a, why do they represent the impulse as having a finite height of 1/2 in Fourier analysis?

Have not touch Fourier Transform for a long time. Far as I remember a dirac delta function is represented by and infinite amount of frequency components after Fourier Transform which means it is flat response on the FT graph with no distinct frequency peak stand out. You have to add all the frequencies together so the final amplitude is high.

I think you'll have better luck going to either Classical Physics or go to ODE/PDE sub-forum here where people there don't worry about producing tangible result and spend all the effort talking about definition and theory!:smile:
 
how can I move this thread to that forum?
 
frenzal_dude said:
how can I move this thread to that forum?

Re-post and bag for forgiveness when you get a warning for posting the same post in two different area:bugeye:

OR

Change the wording and pray the moderator do not recognize it!:smile:

BTW, do you follow about the broad band frequency components in FT so even if individual frequency component is only 1/2 height, but if summing infinite frequencies together, it is possible to get an infinite amplitude at one point.
 
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