Find the Fourier Transform of the function t*(sent/pi*t)^2

In summary, the given function f(t) is equal to the product of the given function g(t) and itself, where g(t) is defined as g(t)=\frac{sen(t)}{t\pi}. To find the Fourier transform of f(t), we can use the convolution property and the derivative property of the Fourier transform. This leads to the result of F(\omega) = \frac{1}{4\pi^2}((\omega-2)H(\omega-2)-2\omega H(\omega)+(\omega+2)H(\omega+2)), which can also be obtained by using the derivative formula 203 from the Wikipedia page on Fourier transforms. The derivative of F(\omega) can then
  • #1
Wtfkeado
3
0

Homework Statement


Find the FT of the following signal

The function is: [tex] f(t) = t(\frac{sen(t)}{t\pi})^2 [/tex]

Homework Equations


Fourier transform: [tex] F(\omega)= \int_{-\infty}^\infty f(t)e^{-jt\omega} [/tex]

My attempt began with this Fourier transform, and that's my goal:

[tex] F[tf(t)]= jF'(\omega) [/tex]

The Attempt at a Solution


English is not my first language but i'll do my best to explain my attempt.

With [itex] F[tf(t)]= jF'(\omega) [/itex] being [itex] f(t)=(\frac{sen(t)}{t\pi})^2 [/itex].

It was clear that i had to find the Fourier transform F(ω) of f(t) for further derivation and multiplication with "j" to finish the problem, so i said that if [itex] g(t)=\frac{sen(t)}{t\pi} [/itex], it would be [itex] f(t) = g^2(t) = g(t)g(t) [/itex] so... that F(ω) that i need is the FT of a product.

So i concluded that the FT of f(t) it's the convolution of the FT of:
[itex] g(t)=\frac{sen(t)}{t\pi} [/itex] with itself, in other words --> [itex] G(\omega)*G(\omega) = F(\omega) [/itex]

So in definitive, i need the FT of [itex] g(t)=\frac{sen(t)}{t\pi} [/itex]. (if I'm not wrong)

I didn't know how to calculate G(ω) directly but i can try to solve G'(ω) and then integrate the result, so i did this:

[tex] \frac{dG(\omega)}{d\omega}= \int_{-\infty}^\infty \frac{sen(t)}{t\pi}\frac{de^{-jt\omega}}{d\omega}dt = \int_{-\infty}^\infty \frac{sen(t)}{t\pi}(-jt)e^{-jt\omega}dt = \frac{-j}{\pi}\int_{-\infty}^\infty sen(t)e^{-jt\omega}dt [/tex]

[tex] \frac{-j}{\pi} \int_{-\infty}^\infty \frac{e^{jt}-e^{-jt}}{2j}e^{-jt\omega}dt = \frac{-1}{2\pi} \int_{-\infty}^\infty e^{jt-jt\omega}-e^{-jt-jt\omega}dt = \frac{-\delta(\omega + 1) + \delta(\omega - 1)}{2\pi} = G'(\omega) [/tex]

Now i integrate G'(ω), the particularity of this is that if H(ω) is the Heaviside function, and δ(ω) is delta dirac's function i can make an equation that says that:

[itex] H'(\omega)=\delta(\omega) \quad then \quad H(\omega) = \int \delta(\omega) [/itex]
(I hope this is ok (?))

So i have at last G(ω):
[tex] G(\omega) = \frac{-H(\omega + 1) + H(\omega - 1)}{2\pi} [/tex]

So i'll be honest, at this point, i didn't know how to do the convolution by myself (i'm learning by myself, the teacher's class was just scratching the surface of the theme so i don't understand it fully, but even so, this is part of a homework and costs points of it), so i consulted with wolfram alpha, here's the link --> http://www.wolframalpha.com/input/?...fx&f4=y&f=ConvolveCalculator.variable2\u005fy

The result was [tex] F(\omega)= G(\omega)*G(\omega) = \frac{1 }{4\pi^2}((\omega-2)H(\omega-2)-2\omega H(\omega)+(\omega+2)H(\omega+2)) [/tex]

Nevermind. I made a huge mistake so i edited my post, i need to derive that F(ω) to obtain F'(ω) and fulfill the TF that i defined in the beginning [itex] F[t(\frac{sen(t)}{t\pi})^2]= jF'(\omega) [/itex]. But this is ok? all that i did? i need some orientation... and there's another way to do all of this?
 
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  • #2
I guess that "sen" is your symbol for the sine?
The fast track would be to use formula 203 of this wikipedia page:

http://en.wikipedia.org/wiki/Fourier_transform

The derivative of a triangular function should not be a problem!
 
  • #3
maajdl said:
I guess that "sen" is your symbol for the sine?
The fast track would be to use formula 203 of this wikipedia page:

http://en.wikipedia.org/wiki/Fourier_transform

The derivative of a triangular function should not be a problem!

Yeah, that's my sine sorry, in spanish it's "seno" so i use sen, my apologies if the notation was confusing, thank you. And... the reason why i didn't use the formula 203 is because in the remarks of the formula, they clarify that their sinc(x) is defined as
[tex] sinc(x) = \frac{sin(x\pi )}{x\pi} [/tex] And mine would be [tex] sinc(x) = \frac{sin(x)}{x} [/tex] So i preferred to not touch that definition. But can i use that formula?
 
  • #4
Of course, you can use that formula.
You simply need to re-arrange it a little bit.
Make a change of variable y = Pi x and re-write formula 203 with your own variable.

Also, you may like to derive formula 203 for your own training, which should not be too difficult.
Doing so, you may also come close to solve your problem fully by your own means which is more fun.
 
  • #5
maajdl said:
Of course, you can use that formula.
You simply need to re-arrange it a little bit.
Make a change of variable y = Pi x and re-write formula 203 with your own variable.

Also, you may like to derive formula 203 for your own training, which should not be too difficult.
Doing so, you may also come close to solve your problem fully by your own means which is more fun.

Hahaha yes, the feeling after you complete something that you worked on for hours straight is irreplaceable, thank you again! so in my case, f(t) being: [tex] \frac{sin(t)}{t\pi}\quad if \quad y=t\pi \quad then \quad t=\frac{y}{\pi} --> f(\frac{y}{\pi}) = (\frac{sin(\frac{y}{\pi})}{\frac{\pi}{\pi}y})^2 = (\frac{sinc(\frac{y}{\pi})}{\pi})^2 = \frac{(sinc(\frac{y}{\pi})^2)}{\pi^2} [/tex] Then, using the formula 203 (non unitary, angular frequency) my result is: [tex] F(\omega) = \frac{1}{\frac{1}{\pi}}tri(\frac{\omega}{2\pi \frac{1}{\pi}}) = \pi tri(\frac{\omega}{2}) [/tex] And it's derivative is: [tex] F'(\omega) = \pi \frac{ rect(\frac{\omega +1}{2}) - rect(\frac{\omega -1}{2})}{2} [/tex] Being "tri" the triangular function and "rect" the rectangular.

And now i apply it to my initial transform. I suppose that that's ok isn it?
 
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FAQ: Find the Fourier Transform of the function t*(sent/pi*t)^2

What is the definition of Fourier Transform?

The Fourier Transform is a mathematical operation that decomposes a function into its constituent frequencies. It is commonly used in signal processing, image processing, and other areas of mathematics and engineering.

How do you find the Fourier Transform of a function?

To find the Fourier Transform of a function, you need to integrate the function multiplied by the complex exponential function e^(-i2πft), where f is the frequency variable. This integral is known as the Fourier Transform integral.

What is the Fourier Transform of t*(sent/pi*t)^2?

The Fourier Transform of t*(sent/pi*t)^2 is a complex function defined by the integral ∫t*(sent/pi*t)^2*e^(-i2πft)dt. It cannot be expressed in a simple closed form, but can be evaluated numerically using various numerical integration techniques.

What is the physical interpretation of the Fourier Transform?

The physical interpretation of the Fourier Transform is that it represents the frequency components of a signal or function. It allows us to analyze and understand the frequency content of a signal, and is often used to filter and manipulate signals in various applications.

What are some common applications of the Fourier Transform?

The Fourier Transform has numerous applications in various fields, including signal processing, image processing, data compression, audio and video processing, and differential equations. It is also used in solving mathematical problems and in physics and engineering for analyzing and understanding systems and signals.

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