Adventures in Parallel Dimension #1729 II

Celebrating the success of parallel dimension #1729's discovery of the Biggs Hoson , CALVIN National Laboratories received a large amount of money and decided to build a REALLY big recreational room with a home theater.

The main features are a huge w = 100 m w=100 \text{ m} wide TV, and a state of the art sound system driven in phase at 1000 W RMS 1000\text{ W RMS} that emits from directly below either end of the TV at a wavelength of λ = 1 m \lambda=1\text{ m} . A d = 1 km d=1\text{ km} long couch is going to be placed parallel to the TV at a distance of l = 10 m l=10\text{ m} from the front end of both speakers.

The architects failed to consider that the material used will cause everything in the room to absorb all of the sound that hits it, so all that anyone will hear are the sound waves directed exactly towards them from the pair of speakers. The physicists there, having a good sense of humor, have decided to play a joke on Greg by assigning him a spot on the couch where he won't be able to hear anything being emitted from the speakers. How many possible spots on the couch are there to place Greg?

Details and Assumptions:

  • Assume that the speakers have range to reach every spot on the couch.
  • Greg is part of a previously failed cloning experiment, so now he's a point mass.
  • The speed of sound through air in parallel dimension #1729 is 340.29 m/s . 340.29 {\text{ m/s}}.
  • Image is not drawn to scale.


The answer is 200.

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1 solution

Brandon Monsen
Jan 27, 2017

The speakers are in phase when they emit sound, but since sound takes time to reach its destination, a path difference will cause the sound waves to be out of phase. Let's call the phase difference ϕ \phi , and the path difference δ \delta . Then ϕ = 2 π δ λ \phi=2\pi \frac{\delta}{\lambda} .

It is trivial that the point on the couch directly in front of the center of the TV will have maximum constructive interference, and thus is our 0 t h 0^{th} order principal maximum. Using this as our base point, call this y = 0 y=0 , where y y is the distance to the right of the 0 t h 0^{th} order maximum while facing the TV. We can then use Pythagorean Theorem to determine the relative phase difference as follows;

y speaker 1 = 50 m , y speaker 2 = 50 m δ = 100 + ( y + 50 ) 2 100 + ( y 50 ) 2 ϕ = 2 π ( 100 + ( y + 50 ) 2 100 + ( y 50 ) 2 ) . \begin{array}{c}\\ y_{\text{speaker 1}}=50\text{m}, \quad y_{\text{speaker 2}}=-50\text{m} \\ \delta=\sqrt{100+(y+50)^{2}}-\sqrt{100+(y-50)^{2}} \\ \phi=2\pi \left( \sqrt{100+(y+50)^{2}}-\sqrt{100+(y-50)^{2}} \right). \end{array}

In order to obtain complete destructive interference, the two speakers must have a relative phase difference of ϕ = π + 2 π k \phi=\pi+2\pi k for some k Z k \in \mathbb{Z} . We get;

1 2 + k = 100 + ( y + 50 ) 2 100 + ( y 50 ) 2 . \begin{array}{c}\\ \frac{1}{2}+k= \sqrt{100+(y+50)^{2}}-\sqrt{100+(y-50)^{2}}. \end{array}

Note that k ( y ) k(y) is a strictly increasing function over the range used in the problem; 500 y 500 -500\leq y \leq 500 ; so we can obtain all possible values of k k by looking at the extreme values of k k and then counting the number of integers that lie between those extrema.

k ( 500 ) = 100 + ( 500 + 50 ) 2 100 + ( 500 50 ) 2 1 2 99.47 k ( 500 ) = 100 + ( 500 + 50 ) 2 100 + ( 500 50 ) 2 1 2 100.47. \begin{array}{c}\\ k(500)=\sqrt{100+(500+50)^{2}}-\sqrt{100+(500-50)^{2}}-\frac{1}{2}\approx 99.47 \\ k(-500)=\sqrt{100+(-500+50)^{2}}-\sqrt{100+(-500-50)^{2}}-\frac{1}{2}\approx -100.47. \end{array}

Hence our range of integral k k is 100 k 99 -100 \leq k \leq 99 , and so there are 200 \boxed{200} possible values of k k , each of which correspond to a point of complete destructive interference.

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