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- [Voiceover] If two waves overlap
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in the same medium, we say that
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there's wave interference.
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So this box here could represent a speaker
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and this could be the
sound wave it generates
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or it could represent a
laser and this would be
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the light wave it generates or it could be
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some sort of ripple
tank generator and this
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is the water wave it generates.
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Regardless, if you had a second source
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of a wave and these were to overlap,
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you'd cause wave interference and what
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that would look like would
be something like this.
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So let's say these are speakers.
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I like thinking about
it in terms of speakers,
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I think it's easy to think about
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and I put this speaker right next
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to the first speaker, side-by-side.
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So they'd be creating sound waves
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in this region and I wouldn't really have
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two sound waves necessarily.
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You can think of it as just having
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one total sound wave and how would we
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find the size of that total sound wave?
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Well if I put an axis in here.
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The axis will make it
easier to think about this.
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I'm going to put an axis
through here like this
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What I can do is I can
just ask myself this,
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I'm going to say, what was the value
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of the first wave, so I'm going
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to take that value.
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What was the value of second wave
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and I'm just going to add them up.
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To get the value of the total wave,
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I'd take that value of the first wave
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plus the value of the second wave
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and well I'd just get double in this case.
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I can come over to here okay.
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The value here plus the value there,
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I get double that point.
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It's not going to be as high
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because they weren't as high..
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Then over here I got zero
and zero is just zero.
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and you start to see what's happening.
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I can come down here very low
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or very negative and I
get double that down here
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and if I were to trace this out,
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what I would get is one
big total sound wave
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that would look like this.
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So these have been amplified.
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So that's one possibility.
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When two waves overlap,
you can get this case
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where the peaks match the peaks
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and the valleys match the valleys
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and you get constructive interference.
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So notice how each valley matches
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the valley, each peak matches the peak
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and this is called,
Constructive Interference
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because these constructively combine
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to form one bigger wave.
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So this is Constructive Interference.
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So what would you hear?
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If your ear was over here somewhere
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waiting to hear this sound.
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What you'd actually hear is a loud note.
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This would be much louder than it was.
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It would be twice as loud in fact.
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Which makes sense.
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You've got a second speaker in here.
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It's twice as loud.
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That makes sense.
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What's a little bit harder to understand
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is you can also have something called,
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Destructive Interference.
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What would that look like?
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Well, imagine you had two speakers
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but they looked like this so that the peak
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of the first one lined
up not with the peak
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of the second one but with the valley
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of the second one and the valley of
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the first one lined up with the peak
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of the second one.
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These are out of phase we say.
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Before, when they looked like this.
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These waves we say are in phase,
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because they look identical.
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The peaks match up with the peaks.
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The valleys with the valleys.
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These are out of phase.
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How far out of phase are they?
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We say that these are
180 degrees out of phase.
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So these are 180 degrees out of phase.
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The phase refers to what point on
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the wave cycle is the wave at
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and these two are starting
completely separately
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which is 180 degrees.
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You might think that means 360
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but think about it.
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If you turn around 360 degrees,
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you're actually back where you started.
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If we tried to make these 360 degrees
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out of phase, they'd look identical again
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because I've moved on
so far through a cycle
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that's it's back to where it started
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in the first place.
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So I want to move it 180
degrees out of phase.
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That's exactly the opposite
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So that you get peak lining up with valley
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or if you like radions, this is called
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pi out of phase because pi and 180
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are the same angle.
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Alright so what happens here
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if I take these two speakers?
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I'm going to take this second speaker
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and I line it up right
next to the first speaker.
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I get something that looks more like this.
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Look at how weird this looks.
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These are completely out of phase
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and what's going to happen is
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if I add my little axis to
help me think about this.
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I'm going to add an axis
straight through here.
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Now I play the same game.
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What total wave do I end up with?
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Well, I take this value.
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I'm going to add up the
values just the same.
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I take the value of the first wave
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plus the value of the second wave.
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I add those up, one's a positive
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and one's a negative I get zero
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and then over here zero plus zero is zero
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and then the valley of the first wave
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is lining up with the
peak of the second wave
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and if I add these two points up,
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I get zero again and you probably see
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what's going to happen.
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I'm just going to get a flat line.
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I'm going to get a flat line and I'm
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going to get no wave at all.
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These two waves cancel and so we call this
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not Constructive Interference
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but Destructive Interference
because these have
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destructively combined
to form no wave at all
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and this is a little strange.
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How can two waves form no wave?
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Well, this is how you do it.
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And what would our ear here if we had
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our ear over in this area again,
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and we were listening.
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If I just had one
speaker, I'd hear a noise.
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If I just had the second speaker,
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I'd hear a noise.
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If I have both the first and second
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speaker together, I don't hear anything.
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It's silent, which is hard
to believe but this works.
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In fact, this is how noise canceling
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headphones work if you take a signal
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from the outside and you send in
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the exact same signal but flipped.
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Pi out of phase or 180
degrees out of phase.
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It cancels it and so you can fight noise
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with more noise but exactly out of phase
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and you get silence in here, or at least
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you can get close to it.
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Now you might be wondering how do we
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get a speaker to go 180
degrees out of phase?
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Well it's not too hard.
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If you look at the back of these speakers.
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Let me make a clean view.
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If you look at the back of these speakers,
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there will be a positive terminal
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and a negative terminal or at lease inside
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there will be and if you can swap
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the positive terminal
for the negative terminal
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and the negative terminal
for the positive terminal,
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then when one speaker's
trying to push air forward,
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there's a diaphragm on this speaker
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moving forward and backwards.
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When one speaker is
trying to push air forward
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the other speaker will be trying
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to pull air backwards and the net result
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is that the air just doesn't move
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because it's got equal and opposite
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forces on it and since
the air just sits there,
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you've got no sound wave because
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air has to oscillate
to create a sound wave
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and you get Disruptive Interference.
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So that's how you can create a speaker
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pi out of phase.
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You might be wondering, I don't want
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to mess with the wires on the back
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of my speaker in fact, you shouldn't
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so you don't get shocked but if I've got
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two speakers in phase
like this, I'm stuck,
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I can't get Destructive Interference
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but yeah you can.
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Even if you don't mess with the wires,
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and don't, don't try this at home,
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you can still take this speaker,
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remember before when these where
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in phase we'd just line them up like that,
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Constructive Interference but I don't
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have to put them side-by-side.
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I can start one speaker
a little bit forward
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and looks what happens.
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We start to get waves
that are out of phase.
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So my question is how far forward
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should I move this speaker to get
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Destructive Interference
and we can just watch.
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So I'm just going to try
this and when we get to
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this point there, now we're out of phase.
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Now I have Destructive Interference
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and so how far did I
move my speaker forward?
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If we look at it, here was the front
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of the speaker originally, right there.
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Here's the front of the speaker now.
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If you look at this wave, how much
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of a wavelength have I moved forward.
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The amount of wavelength that you had
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to move forward was 1/2 of a wavelength.
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So if you take two speakers that are
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in phase and you move one
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1/2 a wavelength forward you get
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Destructive Interference again.
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Again, if my ear's over here, I'm not
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going to hear anything.
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Even though these two waves started off
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in phase, move one 1/2
a wavelength forward,
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they line up so that it's Destructive,
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I get no noise but if I take this away.
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We go back to the beginning here.
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Take my speaker, we start over.
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If you move it forward a whole wavelength,
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so I take this here, keep moving it,
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keep moving it and then
Destructive Interference
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Whoa, here we go, Constructive
Interference again.
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That's a whole wavelength.
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So if you move it forward
a whole wavelength.
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Look, there's one whole
wavelength forward.
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So the front of the speaker was here
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now the front of the speaker's here.
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This is an entire wavelength.
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I get Constructive Interference.
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Now I'm going to hear a loud sound again.
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I'm going to hear twice the noise
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that there would be if
I just had one speaker.
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So the moral of this story is that
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even if you have speakers
that are in phase,
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you can get Destructive Interference
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depending on the difference in the length
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that these two waves travel.
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In other words wave two
is traveling this far
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to get to my ear.
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I'm going to call that x2 and wave one
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is traveling this far to get to my ear.
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I'm going to call that x1.
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If I took the difference
between these two,
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I'd be finding the path length difference.
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The difference in path lengths that
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these waves are traveling and that
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would be this amount.
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This is the difference right here.
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I'm going to call it delta x because
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it's the magnitude of the difference
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between these two lengths and we saw
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that if this equals
lambda it was constructive
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and if it equaled a 1/2 a lambda
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it was destructive but those
aren't the only values.
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We can write down an
important result here.
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If delta x, the path length difference was
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lambda or it turns out 2 lambda will work
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or 3 lambda, imagine
moving the second speaker
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one more whole wavelength.
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Well, you'd be perfectly
back in phase again
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because you'd align back up perfectly
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or 3 whole wavelengths
again, perfectly in phase.
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Any integer wavelength including zero
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because zero is just the case where
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the speaker was right next to speaker one.
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Where these two speakers were lined up
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right next to each other,
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you'll get Constructive Interference.
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The waves line up perfectly,
it's going to be constructive
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and we saw if, delta x
equals a 1/2 wavelength
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it was destructive but
that's not the only case.
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Any odd 1/2 integer here.
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So I can't do 2 over 2 because that
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would be lambda again.
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I could do 3 lambda over
2 or 5 lambda over 2
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or 7 lambda over 2.
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Any of these will give me
Destructive Interference
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because they'll cause these peaks
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to match up with valleys.
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The whole thing would flat line.
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I'd get no sound.
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This is an important result.
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If you've got two speakers that are
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starting off in phase.
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In other words they both
start off the same way
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and by that I mean one speaker sends out
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it's wave going up, the other
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sends out it's wave going up.
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There both at the same cycle.
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If the only difference is
the path length difference,
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this is an important result that let's you
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determine whether there's constructive
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or destructive interference
but you might ask,
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hold on, what if...
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See this was assuming there was no phase
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difference to start off with.
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What if you did the old switcheroo
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on the back of one of these speakers
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and you swapped the positive end
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for the negative end so
instead of coming out
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upward, the second one
was coming out downward.
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Then what would happen?
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Well you might be able to guess.
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Now, this results just going to flip-flop.
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In other words, if I
look at this case here
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Look at, now we start off with speakers
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that are out of phase to begin with.
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This time, if I start off with zero
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path length difference, I get destructive
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destructive instead of constructive.
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If I move this a whole wavelength forward,
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there's a whole wavelength,
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I get destructive again.
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Two wavelengths forward,
destructive again.
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Three wavelengths forward would be
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destructive again and so
the integer wavelength
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this time are going to
give me destructive.
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What about the half integers?
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Let's see, I'll go forward
a 1/2 a wavelength.
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Look at this, perfectly in phase.
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It's going to be constructive.
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How about if I go 3 1/2 of a wavelength.
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Again, perfectly in phase, constructive.
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So, in this case it turns
out if you start off
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with speakers that were
already phase shifted.
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If one speaker is pi
shifted from the other
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then we got another result here.
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We've got that...
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Well actually I'll just go back to my
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previous result, it's easier.
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We can just add a little addendum here if
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if one speaker is pi phase shifted,
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from the other speaker and remember
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these don't have to be speakers.
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They could be any wave source.
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If one speaker's a pi phase shift
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from the other speaker then
you just flip-flop this.
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Then you just take this rule and now
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these give you constructive right here.
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These would give you constructive
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and these up here would
give you destructive
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and so the whole thing just gives you
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the opposite result.
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Now the whole integer
wavelengths give you destructive.
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The 1/2 integer wavelengths
give you constructive
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and I have to impress upon you the idea
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that this does not just
apply for speakers.
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This applies for light and some sort of
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double slit experiment or light in
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a thin film experiment or sound
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with speakers or water waves.
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Any time that's the case, this rule holds
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in fact, this is the fundamental rule
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for almost all wave interference aspects.
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Is that the path length difference
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along with whether
there's a pi phase shift,
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a relative pi phase shift between the two
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will determine whether you get
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constructive or destructive interference.