Amplitude in plane x=y from two speakers placed on x and y axes.

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SUMMARY

The discussion focuses on calculating the amplitude of sound waves in the plane defined by x=y, generated by two speakers located at (-L, 0, 0) and (0, -L, 0). The wave equations provided are f_x and f_y, which describe the sound waves emitted from each speaker. The user attempts to combine these equations to find the resultant amplitude in the specified plane but is confused about the implications of the z-coordinate and how to simplify the equations for the x=y plane. The key takeaway is that the amplitude can be derived from the real part of the combined wave function, but further clarification on the treatment of the z-coordinate is necessary.

PREREQUISITES
  • Understanding of wave equations and complex exponentials
  • Familiarity with sound wave propagation and amplitude calculations
  • Knowledge of coordinate systems in three-dimensional space
  • Basic grasp of phase differences in wave mechanics
NEXT STEPS
  • Explore the derivation of amplitude in wave interference scenarios
  • Study the implications of cylindrical wave propagation in three dimensions
  • Learn about phase shifts and their effects on wave superposition
  • Investigate the mathematical treatment of waves in the x=y plane
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Students and professionals in physics, particularly those studying wave mechanics, sound engineering, or acoustics, will benefit from this discussion.

Saraphim
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Homework Statement


Two speakers at (x,y,z)=-L,0,0 and (x,y,z)=(0,-L,0)

Find the amplitude at all positions in the plane x=y

Homework Equations


The waves are given by:

\tilde{f}_x(\overline{r},t)=\frac{A}{r_x} e^{i(kr_x-\omega t)}

\tilde{f}_y(\overline{r},t)=\frac{A}{r_y} e^{i(kr_y-\omega t+\delta)}

And the amplitude A is real.

The Attempt at a Solution


I'm unsure how to proceed here, at least with finding the amplitude in the plane itself. I'm thinking that the amplitude for all points must be given by the real part of

\tilde{f}(\overline{r},t)=\tilde{f}_x+\tilde{f}_y=Ae^{-i \omega t}\left( \frac{1}{r_x} e^{i kr_x} + \frac{1}{r_y} e^{i(kr_y+\delta)}\right)

But how do I go from here and to only the x=y plane? Do I just set r_x=r_y? How does this carry any information about z? I think I just need a nudge in the right direction.
 
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To elaborate a bit, what is stumping me is that both functions completely discard any information about z, and if I take, for instance, \tilde{f}_x((x,y,z),t) for any set values of (x,y), then the result doesn't depend at all of z! This would make the wave propagate as a cylinder with infinite z-length. Am I going insane?
 
Wow, okay, that was utter nonsense. I've now managed to confuse myself to the point where I don't know what I'm doing.
 

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