Root mean square (RMS) of a sinc function

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SUMMARY

The root mean square (RMS) value of the sinc function is determined to be zero due to its aperiodic nature, which results in finite total energy spread over an infinite time interval. The RMS is defined as f_{rms} = √{lim_{a→∞} (1/2a) ∫_{-a}^{a} f(x)² dx}. The integral for the sinc function, ∫_{-a}^{a} (sin² x / x²) dx, converges to a finite value, leading to an RMS of zero. Discussions also highlight the challenges of approximating the sinc function, suggesting that while it can be approximated using RMS, the function remains non-square-integrable.

PREREQUISITES
  • Understanding of root mean square (RMS) calculations
  • Familiarity with the sinc function and its properties
  • Knowledge of integral calculus, specifically improper integrals
  • Basic concepts of periodic and aperiodic functions
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  • Research the properties of the sinc function in signal processing
  • Learn about the implications of aperiodic functions in Fourier analysis
  • Explore techniques for approximating non-square-integrable functions
  • Study the applications of RMS in various engineering fields
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Mathematicians, engineers, and physicists interested in signal processing, particularly those working with sinc functions and RMS calculations.

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Given that the root mean square (RMS) of a sine function is as follows:

RMS of (a*sin(\omega*r) = a / \sqrt{}2

Let a = 1/\omega

Thus

RMS of ((1/\omega)*sin(\omega*r)) = 1 / (\omega*\sqrt{}2)

But for sinc(\omega*x), what is formula for the RMS?
 
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The rms value of sinc is zero.

I'll define rms as
f_{rms} = \sqrt{ \lim_{a \to \infty} \frac{1}{2a} \int_{-a}^{a} f(x)^2 \,dx }.
Let's find the rms for sinc(x). The integral here is
\int_{-a}^{a} \frac{\sin^2 x}{x^2} \,dx
= \int_{-a}^{-1} \frac{\sin^2 x}{x^2} \,dx + \int_{-1}^{1} \frac{\sin^2 x}{x^2} \,dx + \int_{1}^{a} \frac{\sin^2 x}{x^2} \,dx
\le \int_{-a}^{-1} \frac{1}{x^2} \,dx + \int_{-1}^{1} 1 \,dx + \int_{1}^{a} \frac{1}{x^2} \,dx
= 4 - \frac2a < 4.

Thus, the rms value of sinc is
\sqrt{ \lim_{a \to \infty} \frac{1}{2a} \int_{-a}^{a} \frac{\sin^2 x}{x^2} \,dx } \le \sqrt{ \lim_{a \to \infty} \frac{1}{2a} 4 } = 0.
 
Thanks
 
I understand the case when a approaches infinity, but what about the case where "a" is a finite number?
 
redtree said:
I understand the case when a approaches infinity, but what about the case where "a" is a finite number?

The sinc function is not periodic, in other words it's period is infinity. That's why adriank found it's RMS value to be zero. Think of it this way, it's got a finite total energy that is spread over an infinite time interval, the result is an RMS value of zero.

In many ways it doesn't really make a lot of sense to even talk about the RMS value of an aperiodic function like that. What exactly is your application?
 
I want to find a good approximation for the following function:
a = k * sinc( pi k r) = sin (pi k r) / (pi r)

One approximation would be the following
a = 1 / (pi r)

But I think a better approximation is based on RMS. My feeling is that the sinc funciton above is a periodic function, though with decreasing amplitude as a function of r and therefore can be approximated using RMS.
 
Well, the rms value of sin is 1/\sqrt{2}, so you might guess
a = \frac{1}{\sqrt{2} \lvert \pi r \rvert}.
It doesn't seem very useful though. It's not square-integrable, for instance.
 

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