Help finding Fourier Transform

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Homework Help Overview

The discussion revolves around finding the Fourier Transform of the function f(t) = cos(αt) / (t² + β²). Participants explore the integration process and the application of contour integration techniques.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the substitution of the cosine function using Euler's formula and the subsequent manipulation of the integral. There are questions about the appropriate contour for integration and the handling of poles in the complex plane.

Discussion Status

Some participants have offered guidance on using contour integration and the residue theorem, while others are reflecting on their understanding of the technique. There is a recognition of the need to clarify certain assumptions and methods before proceeding with the problem.

Contextual Notes

Participants note that the function is not periodic and that the integration should not be over the unit circle. There is also mention of the need to work through simpler examples to build confidence in applying the techniques discussed.

jtleafs33
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Homework Statement


Find the Fourier Transform of:

f(t)=\frac{cos(\alpha t)}{t^2+\beta^2}

Homework Equations



F(\omega)=\frac{1}{2\pi}\int^{∞}_{-∞}\frac{cos(\alpha t)exp(i \omega t)}{t^2+\beta^2}

The Attempt at a Solution


I start with:

cos(\alpha t)=\frac{exp(i \alpha t)+exp(-i \alpha t)}{2}

Substituting this in, I get:

F(\omega)=\frac{1}{4\pi}\int^{∞}_{-∞}\frac{exp(it(\alpha+\omega))+exp(it(\omega-\alpha))}{t^2+\beta^2}

From here I know I should be able to get this in the form of some delta functions but I can't figure out the manipulation. I'd appreciate any help!
 
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jtleafs33 said:

Homework Statement


Find the Fourier Transform of:

f(t)=\frac{cos(\alpha t)}{t^2+\beta^2}

Homework Equations



F(\omega)=\frac{1}{2\pi}\int^{∞}_{-∞}\frac{cos(\alpha t)exp(i \omega t)}{t^2+\beta^2}

The Attempt at a Solution


I start with:

cos(\alpha t)=\frac{exp(i \alpha t)+exp(-i \alpha t)}{2}

Substituting this in, I get:

F(\omega)=\frac{1}{4\pi}\int^{∞}_{-∞}\frac{exp(it(\alpha+\omega))+exp(it(\omega-\alpha))}{t^2+\beta^2}

From here I know I should be able to get this in the form of some delta functions but I can't figure out the manipulation. I'd appreciate any help!

If you want to evaluate integrals like that you need to use contour integration. Find the poles, figure out contours and use the residue theorem. Have you done stuff like that?
 
Yes I've used the residue theorem to evaluate contour integrals. We've covered so much in this class I had already forgotten that that technique would work.

Since this involves a 2\pi periodic function, I'd integrate over the unit circle in the complex plane... Use Euler's formula for the cosine substitution to get an integral in Z, and then find the poles and residues, Right?

Thanks Dick!
 
jtleafs33 said:
Yes I've used the residue theorem to evaluate contour integrals. We've covered so much in this class I had already forgotten that that technique would work.

Since this involves a 2\pi periodic function, I'd integrate over the unit circle in the complex plane... Use Euler's formula for the cosine substitution to get an integral in Z, and then find the poles and residues, Right?

Thanks Dick!

That's the general technique alright, but the details are wrong. Your function isn't periodic and you don't integrate over the unit circle. You integrate over part of the real axis and then close the contour in the upper or lower half plane. But sure, review the technique and see how far you get.
 
Right, this acts like a 'sinc' function, so the Jordan contour is the right selection for integration.

So the function is:

f(t)=\frac{cos(\alpha t)}{\beta^2+t^2}

Let:
z=e^{i\alpha t}
dz=i\alpha e^{i\alpha t}dt
cos(\alpha t)=\frac{z+z^{-1}}{2}

Transforming f(t) to f(z)

f(z)=\frac{z+z^{-1}}{2(\beta^2+t^2)} \cdot \frac{dz}{i\alpha z}

So here with this t in the denominator, can I replace it directly with a z, or do I need to use t=\frac{ln(z)}{i\alpha} which I got from the second equation above?

Once I do that, I'll plug into the F.T. integral and find the value from the Residue Thm.
 
jtleafs33 said:
Right, this acts like a 'sinc' function, so the Jordan contour is the right selection for integration.

So the function is:

f(t)=\frac{cos(\alpha t)}{\beta^2+t^2}

Let:
z=e^{i\alpha t}
dz=i\alpha e^{i\alpha t}dt
cos(\alpha t)=\frac{z+z^{-1}}{2}

Transforming f(t) to f(z)

f(z)=\frac{z+z^{-1}}{2(\beta^2+t^2)} \cdot \frac{dz}{i\alpha z}

So here with this t in the denominator, can I replace it directly with a z, or do I need to use t=\frac{ln(z)}{i\alpha} which I got from the second equation above?

Once I do that, I'll plug into the F.T. integral and find the value from the Residue Thm.

That is WAY too fast and sloppy. You aren't going to get anywhere like this. Work out a simple example of this kind of problem first. Integrate e^(it)/(1+t^2) over the real line first. Where are the poles? What's a good contour? If you get that you are probably ready to do to think about the full problem.
 
Okay, taking your advice.

For the example problem,

\int^{∞}_{-∞} \frac{e^{it}}{1+t^2}
We can directly substitute t=z
\oint ^{∞}_{-∞} \frac{e^{iz}}{1+z^2} = \oint ^{\infty}_{-\infty} \frac{e^{iz}}{(1+i)(1-i)}

Now since it's clear to see that f(z)→0 as R→∞, we can integrate over the upper half plane using a semicircular contour.

Only the pole z=i lies inside this contour.

So,

\oint ^{\infty}_{-\infty} \frac{e^{iz}}{(1+i)(1-i)}=2\pi i Res(z=i) = lim_{z→i} (z-i)\frac{e^{iz}}{(z+i)(z-i)}
lim_{z→i}=\frac{2\pi i}{2ie} = \frac{\pi}{e}
 
I figured out what I was doing wrong. I realize now the substitutions I was making from the Euler formula don't work over the real line, those are more suited for integration over the unit circle. Once I chose a better way to transform into an integral in Z, this turned out to be a very simple problem.

Thanks for helping me and for scolding me for blindly pulling a formula out of the book.
 

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