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- [Voiceover] So we started
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with a square wave
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that had a period of two pi,
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then we said, hmm,
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can we represent it
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as an infinite series
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of weighted sines and cosines,
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and then working from that idea,
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we were actually able
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to find expressions
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for the coefficients,
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for a sub zero and a sub n
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when n does not equal zero,
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and the b sub ns.
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And evaluating it for this
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particular square wave,
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we were able to get
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that a sub n is going
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to be equal,
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or a sub zero is going
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to be 3/2,
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that a sub n is going
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to be equal to zero
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for any n
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other than zero,
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and that b sub n
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is going to be equal
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to zero if n is even
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and six over n pi
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if n is odd.
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So one way to think about it,
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you're gonna get your a sub zero,
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you're not gonna have any
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of the cosine terms,
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and you're only going to have
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the odd sine terms.
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And if you think about it
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just visually, if you look
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at the square wave,
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it makes sense
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that you're gonna have
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the sines and not the cosines
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because a sine function
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is gonna look something like this.
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So a sine function is gonna look
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something like this,
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while a cosine function
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looks something like,
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let me make it a little bit neater,
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a cosine function would look
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something like that.
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And so a cosine
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and multiples of cosine
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of two x, cosine of three x,
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is gonna be out of phase,
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while the sine of x,
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or I should say cosine of ts
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and the sines of ts,
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sine two t, sine three t,
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is gonna be more in phase
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with the way this function
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just happened to be.
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So it made sense that our
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a sub ns were all zero
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for n not equaling zero.
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And so based on what we found
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for our a sub zero,
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and our a sub ns,
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and our b sub ns,
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we could expand out
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this actual,
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we did in the previous video,
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what is this Fourier series
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actually look like?
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So 3/2 plus six over pi
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sine of t plus six over three pi
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sine of three t plus
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six over five pi
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sine of five t,
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and so on and so forth.
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And so a lot of you might
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be curious what does this
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actually look like.
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And so I actually just,
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you can type these things
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into Google and it will
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just graph it for you.
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And so this right over here
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is just the first two terms.
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This is 3/2 plus six over pi
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sine of t.
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And notice it's starting
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to look right because our
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square wave looks something
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like, it goes,
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it looks something like this.
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So it's gonna go like that
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and then it's gonna go down
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to zero and then it's gonna go
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up, looks something like that.
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It doesn't have the pis
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and the two pis
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marked off between these
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because it's gonna look
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something like that.
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So even just the two terms,
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it's kind of a decent approximation
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for even two terms,
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but then as soon as you get
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to three terms,
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if you add the six
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over three pi sine of three t
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to the first two terms.
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So if you look at these
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first three terms,
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now it's looking a lot
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more like a square wave.
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And then if you add the next term,
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well, it looks like even more
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like a square wave,
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and then if you add to that
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what we already wrote down here,
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if you were to add to that
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six over seven pi times
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sine of seven t,
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it looks even more
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like a square wave.
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So this is pretty neat.
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You can visually see
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that we were actually able
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to do it.
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And it all kind of just
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fell out from the mathematics.