Ask your own question, for FREE!
Mathematics 10 Online
OpenStudy (lalaly):

Fourier

OpenStudy (lalaly):

@mr.math

OpenStudy (lalaly):

it s ok mr math, thanks anyways:)

OpenStudy (mr.math):

Oh I know the solution -.- My page went down twice!! :(

OpenStudy (mr.math):

I will write again using another browser. I love my solutions to be complete, so sorry for taking so long :)

OpenStudy (lalaly):

oh :-D take your time lol, i am sorry for bothering you xD

OpenStudy (mr.math):

I'm starting to hate Google Chrome. Lets see how Firefox works out for me :D

OpenStudy (mr.math):

So you know the definition of Fourier transform: The Fourier Transform of an integrable function \(f(x)\) is define as \[\large F(\omega)=\int_{-\infty}^{\infty} f(x)e^{-2\pi i x\omega}.\] For our function \(f(x)=e^{-x^2}\), we have \[F(\omega)=\int_{-\infty}^{\infty}e^{-x^2}e^{-2\pi i x \omega}dx.\] The question becomes now how to evaluate this integral?! You probably know the famous Gaussian integral \(\int_{-\infty}^{\infty} e^{-x^2}dx=\sqrt{\pi}\). We will manipulate our integrand to make it of a similar form. \[F(\omega)=\int_{-\infty}^{\infty}e^{-x^2}e^{-2\pi i x \omega}dx=\int_{-\infty}^{\infty}e^{-x^2-2\pi i x \omega}dx=\int_{-\infty}^{\infty}e^{-(x^2+2\pi i x \omega)}dx\] \[=\int_{-\infty}^{\infty}e^{-(x+\pi i \omega)^2-\pi^2\omega^2}dx=e^{-\pi^2\omega^2}\int_{-\infty}^{\infty}e^{-(x+\pi i w)^2}dx.\]

OpenStudy (mr.math):

Now substitute \(u=x+\pi i \omega\) and use Gaussian integral to evaluate the integral above.

OpenStudy (lalaly):

:-D i will do that,, Thankyou soo much Mr math :D youre the best

OpenStudy (mr.math):

You can see this for the integration of exp(-x^2) https://www.youtube.com/watch?v=fWOGfzC3IeY

OpenStudy (mr.math):

if you want! :)

OpenStudy (lalaly):

i know how to find it by normal distribution xD

OpenStudy (mr.math):

I have alwyas known that you're smart!

OpenStudy (lalaly):

haha not as smart as mr math xD

OpenStudy (mr.math):

If I remember well, you study Communication Engineering, right?

OpenStudy (lalaly):

yepp :-D lol you have a good memory

OpenStudy (mr.math):

Only the things about "important" people! ;)

OpenStudy (lalaly):

I feel special now :-$

OpenStudy (mr.math):

Fourier transform has many applications in your field, right?

OpenStudy (mr.math):

I have taken a course in Signals and Systems two semesters ago and I liked it.

OpenStudy (lalaly):

yeah but i am taking a course where fourier transform is solved in mathematics way... and its different from what ive taken in signals and systems and communication -.- i solved this question in a way ,, the professor said he wants it solved in mathematicians way not engineers :S

OpenStudy (mr.math):

Lol, Mathematicians are always the best. Engineers come second so you don't get upset :P

OpenStudy (lalaly):

lol no doubt:P I dont mind coming second after you xD

OpenStudy (mr.math):

Well, I think as long as the solution provides all logical steps needed, it should be enough. I did take Fourier transform in two different courses one of which was this Engineering course I just told you about. I remember in that course we were allowed to use tables, but in a Math course we would have to derive them ourselves in one way or another.

OpenStudy (lalaly):

It is amazing,,, Thanks again :-D ... i wont drive u crazy after this dont worry hehe

OpenStudy (mr.math):

You look more "Arab" in this picture for some reason. I like all you pictures anyways :)

OpenStudy (mr.math):

You're welcome, and good luck!

OpenStudy (lalaly):

lol thats sweet:)

OpenStudy (mr.math):

Important note: I should have used \(f\) instead of \(\omega\) there, because the transform I did was in terms of frequency not angular frequence. You can use \(\omega=2\pi f\) to write it in angular frequency, as you know.

OpenStudy (lalaly):

i appreciate ur help ^_^

OpenStudy (lalaly):

found the easy way :P thought id show it to u let f(x)=e^(-x^2) and let f^ (f-hat) = F \[f'(x)=-2xe^{-x^2}\] take fourier transform of both sides\[F[f'(x)]=-2F[xf(x)]\]we know that \[F[f']=iwF\]and \[\large{F[xf]=iF '}\]so now we have\[iwF=-2iF'\]the i cancels \[wF=-2F'\]now we seperate\[wdw=\frac{-2}{f}dF\]integrate both sides\[\frac{w^2}{2}=-2lnF+C\]take e of both sides\[\large{e^{\frac{w^2}{2}}=e^{lnF^{-2}+C}}\]so simplifying\[\huge{F=C_2e^{-\frac{w^2}{4}}}\]now we find the constant observe F(0)=C_2 so \[C_2=\frac{1}{\sqrt{2 pi}} \int\limits_{-\infty}^{\infty}e^{-x^2}dx\]we know that theat integral =sqrt(pi) so \[C_2=\frac{1}{\sqrt2}\] now \[\huge{F(w)=\frac{1}{\sqrt 2}e^{-\frac{w^2}{4}}}\]hoooooooooooooof lol

OpenStudy (lalaly):

@mr.math

OpenStudy (mr.math):

That's smarter but not easier :-)

OpenStudy (lalaly):

lol maybe :P ... i dont like having so many integrals ... so thats why i tried to find it in another way

OpenStudy (lalaly):

Mr math do u know bivariate random variables?

OpenStudy (mr.math):

I don't think the solution I gave has that many integrals. And I don't know bivariate random variables.

OpenStudy (lalaly):

lol its ok,,, i just wanted to ask a question xD

OpenStudy (mr.math):

If I was doing it with myself, I would just do it like this: \[F(\omega)=\frac{1}{\sqrt{2\pi}}\int_{-\infty}^{\infty}e^{-x^2}e^{-i\omega x}=\frac{1}{\sqrt{2\pi}}\int_{-\infty}^{\infty}e^{-(x+\frac{i\omega}{2})^2-{\omega^2\over 4}}dx\] \[=\frac{e^\frac{-\omega^2}{4}}{\sqrt{2\pi}}\sqrt{\pi}=\large \frac{1}{\sqrt{2}} e^{\frac{-\omega^2}{4}}.\]

OpenStudy (mr.math):

But I like the tricks you used.

OpenStudy (lalaly):

yeah thats shorter hehe,,, ill write down both,, what u did was awesome, i just wanted to share with u what i thought about

OpenStudy (mr.math):

Thanks! What you did is awesome too. Is this a homewrok asignment or what?

OpenStudy (mr.math):

assignment*

OpenStudy (lalaly):

lol yeah something like that :P

Can't find your answer? Make a FREE account and ask your own questions, OR help others and earn volunteer hours!

Join our real-time social learning platform and learn together with your friends!
Can't find your answer? Make a FREE account and ask your own questions, OR help others and earn volunteer hours!

Join our real-time social learning platform and learn together with your friends!