00:01
In this case, we've got three waves interfering with each other.
00:13
First thing i want to do is i want to calculate r here.
00:21
I'm going to call this r sub 2.
00:27
And r sub 2 is going to be using the pythagorean theorem, the square root of 3 squared plus 4 squared.
00:47
Well, that's easy.
00:48
It's a 3 .45 triangle using pythagorean triples 5 .0 meters.
01:01
All right.
01:06
Now, let's look at the phase difference between 1 and 2.
01:27
2.
01:44
Lambda.
01:45
So i'm going to put, well, i'll put lambda down here.
01:51
All right.
01:54
2 pi, speed equals wavelength times frequency.
02:01
So wavelength is speed over frequency.
02:06
So 2 pi f, delta r, which is just r2 minus r1, which is just one.
02:15
So i'm just going to say that that's 1.
02:19
Because it is, over speed.
02:27
This is zero.
02:34
F over v, f over v is one half.
02:49
So the phase difference is pi.
02:58
And so that would be perfect, destructive interference.
03:17
Since speakers one and two are going to destruct each other perfectly.
03:25
The only thing that would remain is the magnitude of three.
03:31
And so the amplitude at this point is just going to be the amplitude of each of the speakers individually, which is a.
03:54
I'm just trying to make sure that they told us that it is a.
03:58
Yeah, a.
04:00
So it's just a.
04:01
B, it's asking me about moving speaker two, and i didn't realize that these were given numbers in the drawing.
04:17
So, uh -oh, they're given numbers in the drawing of one, two, and three...