- #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?
Last edited: