Frequency at which no destructive interference occurs

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prodo123
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Homework Statement



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Two speakers A and B, 2.00 m apart, produce a sine wave at the same frequency and phase. A microphone is placed on the line BC perpendicular to AB, at a distance x from B. The speed of sound is v=344 m/s.

For a frequency ƒ low enough, there will be no destructive interference along the line BC. Find this frequency.

Homework Equations



Let ##r=\sqrt{x^2+2^2}## be the distance from speaker A to the point along the line BC.

##y_{A}(x,t)=A\cos(kr-\omega t)\\
y_{B}(x,t)=A\cos(kx-\omega t)\\
k=\frac{2\pi f}{v}\\
\omega = 2πf##

The Attempt at a Solution



Destructive interference occurs when ##y_{A} = -y_{B}##:

##A\cos(kr-\omega t) = -A\cos(kx-\omega t)\\
A\cos(kr-\omega t) = A\cos(kx-\omega t+(2n-1)\pi)\\
kr = kx+(2n-1)\pi\\
r=\sqrt{x^{2}+2^{2}}=x+\frac{(2n-1)\pi}{k}\\
r=x+\frac{(2n-1)v}{2f}##

For simplicity, let ##C = \frac{(2n-1)v}{2f}##

##r^2 = x^2+4 = x^2+2cx+c^2\\
2cx = 4-c^2\\
x(n) = 2/c - c/2\\
x(n) = \frac{4f}{(2n-1)v} - \frac{(2n-1)v}{4f}##

A previous part of the problem set ƒ = 786 Hz and asked to find points of destructive interference; values for which x(n) > 0 found points of destructive interference at n=1,2,3,4,5, which correlated with the answer in the back.

Since x(n) increased as n→1, I think n=1 is the first point of destructive interference from ∞→x. Therefore if x(1)=0, there are no other point of destructive interference other than the source B itself.

Finding the frequency ##f## for which ##x(1)=0##:

##x(1) = \frac{4f}{v}-\frac{v}{4f}= 0\\
4f=v\\
f=\frac{v}{4} = 344/4 = 86\text{ Hz}##

which is the correct answer in the textbook.I'm having trouble interpreting the equation x(n) that I derived.

1. There are also negative values of x(n) for ##n>5## and ##-4<n\le 0##, and positive values for ##n\le -5## when ƒ=786 Hz. Since x is a point along the continuous line BC, and r is defined for all x, why doesn't the textbook count all nonzero values of x(n) as points of destructive interference? Or if it's looking specifically for ##x>0##, why doesn't it count x(n) for ##n<1##?

2. If x(1) = 0 then isn't B itself a point of destructive interference?

3. x(0) as well as x(1) equals 0 at ƒ=86 Hz. What does this mean?

4. Is my interpretation correct that if the only point of destructive interference is x(1) = 0, speaker B is not able to output any sound since the source itself is destructively interfered?
 

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Hello Prodo, :welcome:

1.) There is indeed symmetry wrt the line AB. I don't have the exact problem statement for
prodo123 said:
A previous part of the problem
however, if it says 'distance from B' then all is well.

2. It sure is.

3. It means that the distance from B is zero when you are at B. That is not what you mean, I suppose :rolleyes:. You mean to say something about ##y_A+y_B##, but your equation for ##y## does not take into account that ##A## also varies with distance.

4. Therefore your interpretation is not correct.
 
BvU said:
Hello Prodo, :welcome:

1.) There is indeed symmetry wrt the line AB. I don't have the exact problem statement for
however, if it says 'distance from B' then all is well.

2. It sure is.

3. It means that the distance from B is zero when you are at B. That is not what you mean, I suppose :rolleyes:. You mean to say something about ##y_A+y_B##, but your equation for ##y## does not take into account that ##A## also varies with distance.

4. Therefore your interpretation is not correct.

Thanks for the reply. The chapter doesn't handle displacement amplitude decay over distance, which is why I held A constant.

The issue is that there's supposed to be reciprocity but the textbook ignores (or denies?) it. The previous part of the question simply says:
At what distances from B will there be destructive interference?
Values of ##x(n)## for n=1,2,3,4,5... give 9.01m, 2.71m, 1.27m, 0.534m, 0.026m which are the five values given as the answer to the problem. I'll give the textbook the benefit of doubt of looking for positive ##x## only, since the diagram shows BC going in the positive-x direction only.
But even so ##x(-5)## results in 0.372m, and ##x(n)## for all ##n\le -5## is positive. Looking at the graph of ##y_A+y_B## these are indeed points where the two waves cancel out.
I'm honestly starting to think the textbook got lazy and didn't bother to write down all the solutions...
 
prodo123 said:
The chapter doesn't handle displacement amplitude decay over distance
But you know from experience.

prodo123 said:
there's supposed to be reciprocity
reciprocity ?

At what distances from B will there be destructive interference?
It does not ask for ##x##, it asks for distances. Distances are alsways positive. They can be to the left or to the right. If this is with 786 Hz, then I don't understand the given answers. Can you explain ?
 
BvU said:
But you know from experience.
Yes, I know from experience but that's not what the question is asking for and including it will give the wrong answer to the problem.

BvU said:
reciprocity ?

It does not ask for ##x##, it asks for distances. Distances are alsways positive. They can be to the left or to the right. If this is with 786 Hz, then I don't understand the given answers. Can you explain ?

Sorry, meant to say symmetry across ##x=0##.

After some discussion and playing around with the graph of ##y_A+y_B## I concluded on the following:
  • Diagram specifically points to the right only. Mathematically negative ##x## exists but the problem ignores that.
  • The textbook is looking for positive distances from ##B## at which total cancellation occurs for all t.
  • The given answers for 786 Hz (9.01m, 2.71m, 1.27m, 0.534m, 0.026m) are the only points on BC where this occurs under the given conditions and ##f=786\text{ Hz}##.
  • Graph of ##x(n)## (treating ##n## as continuous instead of an integer) shows it's a hyperbola, and the textbook's answers correspond to the positive values of the right half of the hyperbola only.
  • If ##f=86\text{ Hz}##, ##x=0## is the only place this occurs.
  • Apparently ##x\ne 0## (the speaker B itself is not a part of BC?), therefore the question considers ##f=86\text{ Hz}## to have no such points on BC even though it occurs at ##x=0##.
The solutions for ##x(n)## outside ##[1,...,5]## are zeroes (total cancellation) of ##y_A+y_B## at time ##t=0##, but do not hold at other values of ##t##. For example, ##x(-5)=0.372## is not a zero at time ##t=10##.

I've decided it's just a really poorly worded question and moved on.
 
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prodo123 said:
##x(n)## for n=1,2,3,4,5... give 9.01m, 2.71m, 1.27m, 0.534m, 0.026m
I find these values if I take ##f = 784## Hz, not 786 ?!
prodo123 said:
Diagram specifically points to the right only. Mathematically negative ##x## exists but the problem ignores that
No. ##x## is a distance, a length. And a length is non-negative.

You wanted to solve ##r=\sqrt{x^{2}+2^{2}}=x+\frac{(2n-1)\pi}{k}## and in order to do so, you squared left and right. Did it occur to you that you introduced wrong answers that way ? Did you check that your ##x(-5) = -x(6)## satisfies the original equation (it does not) ?
 
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BvU said:
I find these values if I take ##f = 784## Hz, not 786 ?!
No. ##x## is a distance, a length. And a length is non-negative.

You wanted to solve ##r=\sqrt{x^{2}+2^{2}}=x+\frac{(2n-1)\pi}{k}## and in order to do so, you squared left and right. Did it occur to you that you introduced wrong answers that way ? Did you check that your ##x(-5) = -x(6)## satisfies the original equation (it does not) ?

Sorry, I got confused, it's for 784 Hz.

Showing that ##x(-5)## is indeed equal to ##-x(6)##:

##x(-5)=\frac{4*784}{344(2(-5)-1)}-\frac{344(2(-5)-1)}{4*784}\\
x(-5)=\frac{3136}{-3784}-\frac{-3784}{3136}\\
x(6)=\frac{4*784}{344(2(6)-1)}-\frac{344(2(6)-1)}{4*784}\\
x(6)=\frac{3136}{3784}-\frac{3784}{3136}\\
-x(6)=\frac{-3136}{3784}-\frac{-3784}{3136}=x(-5)\\
\\
x(-5)=\frac{70065}{185416}\approx 0.37788##

as for ##y_A=-y_B## at time ##t=0##:

##y_A+y_B=0\\
A\cos(\frac{784*2\pi}{344}x(-5))+A\cos(\frac{784*2\pi}{344}\sqrt{x(-5)^2+4})=0\\
\cos(\frac{70065\pi}{40678})+\cos(\frac{377393\pi}{40678})=0\\
0.64329-0.64329=0\\
0=0##

Graph of ##y_A+y_B## showing that 0.37788 is indeed a root:
Screen Shot 2018-04-21 at 1.48.16 AM.png
 

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Here's a comparison of the roots for ##y(x)=y_A+y_B, f=784\text{ Hz}##, assuming an arbitrary amplitude of 1 for both waves, found at different values of ##t##.

The given set of roots include ##x(4)=0.026## and ##x(5)=0.534## (blue); the root in question is ##x(-5)=0.37788## (red).

at ##t=0##:
Screen Shot 2018-04-21 at 2.02.00 AM.png


at ##t=0.8##:
Screen Shot 2018-04-21 at 2.01.47 AM.png


at ##t=1.3##:
Screen Shot 2018-04-21 at 2.05.22 AM.png


which shows ##x=0.37788## to be a root only when ##t=0##, while the given answers hold true for all ##t##.

BvU said:
You wanted to solve ##r=\sqrt{x^{2}+2^{2}}=x+\frac{(2n-1)\pi}{k}## and in order to do so, you squared left and right. Did it occur to you that you introduced wrong answers that way ?

I think you're right about the squaring introducing false answers, but then how would one prove that a root at some time ##t## is also a root for all ##t##?
 

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