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A wave defined by $f(t)=a$ for $t\in (0,T)$ and $f(t)=-a$ for $t\in (-T,0)$ (the wave is $2T$ periodic) is input into a system that transmits angular frequencies $<\omega$ and absorbs those $>\omega$. How might I find the form of the output? Firstly, I am not quite sure what is going on here. Am I supposed to find the Fourier series for $f(t)$ then eliminate the terms whose arguments of the cosines or sines are $>\omega$? But how do I find/express the "form" of the output? Thanks in advance!

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You system is an ideal lowpass filter, so yes you can just remove the frequency components which are greater than the cutoff frequency $\omega$. –  Unreasonable Sin Sep 22 '11 at 18:16
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Is the wave periodic? If so, what is the period? My guess would be $2T$, but it is unclear from your question if the wave is even periodic, or simply a pulse. Also, you probably mean $t\in(0,T)$ and $t\in(-T,0)$, not $x$. –  robjohn Sep 22 '11 at 18:38
    
@robjohn: You are right. Sorry about that. –  I. S. Sep 22 '11 at 19:27
    
@UnreasonableSin: But what is the resulting output solution? –  I. S. Sep 22 '11 at 19:29
    
@I. S.: thanks for correcting the typo. Is the wave $2T$-periodic? –  robjohn Sep 22 '11 at 19:40
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In order to get the Fourier series you'll need to impose the condition that the waveform is periodic, which means it's a square wave with period $2T$. The Fourier series of a square wave is well known:

http://en.wikipedia.org/wiki/Square_wave
http://mathworld.wolfram.com/FourierSeriesSquareWave.html

From that you just remove the terms of the series which have frequency components greater than the cutoff frequency $w$, which results in a truncated series. The resulting filtered waveform will not have the sharp transition at $t = 0$ that the original waveform had, but will instead have rounded edges and a slower transition from $-a$ to $a$.

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Thanks, Unreasonable Sin. :-) –  I. S. Sep 22 '11 at 20:08
    
"The resulting filtered waveform...will instead have rounded edges..." It will? Seems to me it will suffer from Gibbs phenomenon, hence have quite bad behavior around $t=0$. Maybe you meant something else with this remark? –  cardinal Sep 22 '11 at 20:16
    
Maybe squiggly edges is a better way to put it. =) –  Unreasonable Sin Sep 22 '11 at 20:40
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Assuming the wave is $2T$-periodic, it is an odd function, so all of the cosine terms in the Fourier series are $0$. Thus $$ f(t)=\sum_{n=1}^\infty\;b_n \sin\left(\frac{n\pi t}{T}\right) $$ where $$ b_n=\frac{1}{T}\int_{-T}^T f(t)\sin\left(\frac{n\pi t}{T}\right)\;\mathrm{d}t $$ The frequency of each term is $\frac{n}{2T}$, so remove all terms of the sum for which $\frac{n}{2T}>\omega$. Your answer should be a finite sum of sine waves.

Spoiler: If $n$ is even, $b_n=0$. If $n$ is odd, then $b_n=\frac{4a}{n\pi}$. Therefore, $$ \tilde{f}(t)=\sum_{k=0}^{\lfloor T\omega-1/2\rfloor}\frac{4a}{(2k+1)\pi}\sin\left(\frac{(2k+1)\pi t}{T}\right) $$

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Thanks, robjohn. :-) –  I. S. Sep 22 '11 at 20:08
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