Why do power signals have finite power and infinite energy?

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Discussion Overview

The discussion centers around the characteristics of power signals and energy signals, particularly focusing on why power signals have finite power and infinite energy, while energy signals have finite energy and zero power. Participants also explore the representation of these signals through Fourier series and Fourier transforms, raising questions about the conditions under which each representation is applicable.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants state that power signals have finite power and infinite energy, while energy signals have zero power and finite energy.
  • One participant provides an example of a power signal using the function $$f_1(t) = \sin \omega_0 t$$, noting its finite power and infinite energy.
  • Another participant questions the assertion that power signals cannot be represented by Fourier transforms, citing a specific Fourier transform for the sine function.
  • A different participant points out that delta distributions must be considered when discussing the Fourier transform of power signals.
  • One participant argues that it is difficult to prove that all power functions lack Fourier representation, suggesting that periodic functions cannot be represented by Fourier transforms due to the Riemann-Lebesgue lemma.
  • Another participant agrees that power signals are periodic and emphasizes that they can only be represented by Fourier series, not Fourier transforms, due to their non-decaying nature.

Areas of Agreement / Disagreement

Participants express differing views on the representation of power signals through Fourier transforms, with some asserting that such representations are not possible while others provide counterexamples. The discussion remains unresolved regarding the general applicability of Fourier transforms to power signals.

Contextual Notes

Participants mention the Riemann-Lebesgue effect and the nature of periodic functions, indicating that the discussion involves complex mathematical concepts that may not be fully resolved within the thread.

parthj09
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I have read that for
power signals : power = finite and energy = infinite
Energy signals : power = 0 and energy = finite
Can anyone give practical example for this...?
Also we can represent power signal through Fourier series only but not through Fourier trransform..unlike energy signals.. why is that..?
I googled it but didnt get any satisfactory answerReport**
 
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parthj09 said:
I have read that for
power signals : power = finite and energy = infinite
Energy signals : power = 0 and energy = finite
Can anyone give practical example for this...?
Also we can represent power signal through Fourier series only but not through Fourier trransform..unlike energy signals.. why is that..?
I googled it but didnt get any satisfactory answerReport**

For example, take function

$$
f_1(t) = \sin \omega_0 t
$$

This function has "power" ##|f_1|^2 \leq 1##, but "energy"
$$
\int_{-\infty}^{\infty} |f_1|^2\,dt
$$
is infinitely great.

This function does not have ordinary Fourier transform (in terms of Fourier function), because the ordinary Fourier integral does not converge. It has however Fourier series: the series contains only one term, the function itself.
(there is however generalized Fourier transform of ##f_1##, which employs delta distributions).

There are also functions that have infinite "energy" and cannot be represented even by a Fourier series, for example realization of the Ornstein-Uhlenbeck process.
 
Thank you..but i still have one doubt...in your explanation about Fourier transform.
As much as i know Fourier transform do exist for f_1(t) = Asin wt
It would be F_1(f) = iA/2 [(f+fm) - (f- fm)]
taking w = 2 pi fm
Now f_1(t) is a power signal then why its Fourier transform is available?
 
Last edited:
It would be F_1(f) = iA/2 [(f+fm) - (f- fm)]
Haven't you forgot delta distributions in the bracket? With distributions, it is true that one can write generalized Fourier transform even for sin function.
 
Yeah but it still doeant answer my question.. why power signals cannot be represented in Fourier transform?
 
It is hard to prove that all "power" functions do not have Fourier representation. It probably is not true.

Instead, I will show why a function given by Fourier series (which has non-zero average power) cannot be represented via Fourier transform.

Let the function be given by

$$
f(t) = \sum_k c_k e^{ik\omega_0 t}.
$$
It has average "power", or better - average square - equal to
$$
\overline{f^2} = \sum_k |c_k|^2.
$$
The function is periodic and does not decay to zero.

However, any Fourier representation

$$
f(t) = \int_{-\infty}^{\infty} \tilde{f}(\omega)\, e^{i\omega t}\, \frac{d\omega}{2\pi}.
$$
with piecewise continuous ##g(\omega)## has to decay to 0 as ##t\rightarrow \pm \infty## (Riemann - Lebesgue effect).

Hence the Fourier series ##f(t)## cannot be represented by any piecewise continuous function ##\tilde f(\omega)##.

This is not a proof, but I think it gives an idea why the Fourier transform does not work for such functions.
 
Yeah thanks for this example.
I did some digging too and found out that all power signals are periodic in nature, and it is impossible to write Fourier transform of periodic signals. They can only be represented by Fourier series.
And also according to you..fourier transforms are supposed to decay..which power signals do not .. so its a win win for us both. :-)
 

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