Please check my solution for this Fourier transform (time diff. Prop.)

YehiaMedhat

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The main question is to transform the following expression: itt2+4\frac{it}{t^2 + 4}
1. Using the symmetry property first: 2πi4e2ω2\pi \frac{i}{4} e^{-2|-\omega|}
2. Then applying the differentiation in time property: iddω[iπ2e2ω]i\frac{d}{d\omega} [\frac{i\pi}{2} e^{-2|\omega|}]
3. Differentiating: π4e2ω\frac{\pi}{4} e^{-2|\omega|}
Is that right, because the solution in the TA's sheet also shows that it's different answer.
 
The main question is to transform the following expression: itt2+4\frac{it}{t^2 + 4}
1. Using the symmetry property first: 2πi4e2ω2\pi \frac{i}{4} e^{-2|-\omega|}
2. Then applying the differentiation in time property: iddω[iπ2e2ω]i\frac{d}{d\omega} [\frac{i\pi}{2} e^{-2|\omega|}]
3. Differentiating: π4e2ω\frac{\pi}{4} e^{-2|\omega|}
Is that right, because the solution in the TA's sheet also shows that it's different answer.
What is the answer in the TA's sheet?
 
2πe2ωu(ω)2\pi e^{-2|\omega|}u(-\omega)
u(ω)u(-\omega) is there because f(t)f(t) is an odd function and we want just negative frequencies.


The main question is to transform the following expression: itt2+4\frac{it}{t^2 + 4}
1. Using the symmetry property first: 2πi4e2ω2\pi \frac{i}{4} e^{-2|-\omega|}
2. Then applying the differentiation in time property: iddω[iπ2e2ω]i\frac{d}{d\omega} [\frac{i\pi}{2} e^{-2|\omega|}]
3. Differentiating: π4e2ω\frac{\pi}{4} e^{-2|\omega|}
Is that right, because the solution in the TA's sheet also shows that it's different answer.
How did you get π4\frac{\pi}{4} in step three?
 
The main question is to transform the following expression: itt2+4\frac{it}{t^2 + 4}
1. Using the symmetry property first: 2πi4e2ω2\pi \frac{i}{4} e^{-2|-\omega|}
2. Then applying the differentiation in time property: iddω[iπ2e2ω]i\frac{d}{d\omega} [\frac{i\pi}{2} e^{-2|\omega|}]
3. Differentiating: π4e2ω\frac{\pi}{4} e^{-2|\omega|}
Is that right, because the solution in the TA's sheet also shows that it's different answer.
If I do the transformation by integration, I get F(ω)=π2e2ωsgn(ω)\displaystyle F(\omega) = \frac{\pi}{2}e^{-2|\omega|} \text{sgn}(\omega)

And because f(t)f(t) is odd, we should include a negative sign to the final answer.

F(ω)=π2e2ωsgn(ω)\displaystyle F(\omega) = -\frac{\pi}{2}e^{-2|\omega|} \text{sgn}(\omega)

And if you will use symmetry, the answer 2πi4e2ω2\pi\frac{i}{4}e^{-2|\omega|} is for it2+4\frac{i}{t^2 + 4}

For itt2+4\frac{it}{t^2 + 4}, the answer should be 2πiω4e2ω2\pi\frac{i\omega}{4}e^{-2|\omega|}
 
F(ω)=π2e2ωsgn(ω)\displaystyle F(\omega) = -\frac{\pi}{2}e^{-2|\omega|} \text{sgn}(\omega)
I did a contour integration, and I got a slightly different result from my first attempt.

Now, I will solve the problem by the Symmetry Property and Differentiation Property.

The main question is to transform the following expression: itt2+4\frac{it}{t^2 + 4}
1. Using the symmetry property first: 2πi4e2ω2\pi \frac{i}{4} e^{-2|-\omega|}
2. Then applying the differentiation in time property: iddω[iπ2e2ω]i\frac{d}{d\omega} [\frac{i\pi}{2} e^{-2|\omega|}]
3. Differentiating: π4e2ω\frac{\pi}{4} e^{-2|\omega|}
Is that right, because the solution in the TA's sheet also shows that it's different answer.
Let g(t)=it2+4\displaystyle g(t) = \frac{i}{t^2 + 4} and f(t)=tg(t)\displaystyle f(t) = tg(t)

The Symmetry Property will give you:

F{g(t)}=G(ω)=2πi4e2ω=πi2e2ω\mathcal{F}\{g(t)\} = G(\omega) = 2\pi \frac{i}{4} e^{-2|\omega|} = \pi \frac{i}{2} e^{-2|\omega|}

Now we can use the differentiation property:

F{f(t)}=F{tg(t)}=F(ω)=idG(ω)dω=ωωπe2ω\displaystyle \mathcal{F}\{f(t)\} = \mathcal{F}\{tg(t)\} = F(\omega) = i\frac{dG(\omega)}{d\omega} = \frac{\omega}{|\omega|}\pi e^{-2|\omega|}

Because f(t)f(t) is an odd function, you need to multiply its Fourier transform by 1-1.

F(ω)=ωωπe2ω\displaystyle F(\omega) = -\frac{\omega}{|\omega|}\pi e^{-2|\omega|}

You can replace the fraction ωω\displaystyle \frac{\omega}{|\omega|} by sgn(ω) or u(ω)\text{sgn}(\omega) \ \text{or} \ u(\omega).

F(ω)=πe2ωu(ω)\displaystyle F(\omega) = -\pi e^{-2|\omega|}u(\omega)

We know that u(ω)=u(ω)\displaystyle -u(\omega) = u(-\omega).

F(ω)=πe2ωu(ω)\displaystyle F(\omega) = \pi e^{-2|\omega|}u(-\omega)

Which is slightly different than TA's sheet answer! TA's sheet answer has a typo, maybe?!
 
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