Wavevector k in Helmholtz Equation

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SUMMARY

The discussion centers on the wavevector k in the context of the Helmholtz equation, derived from the wave equation through separation of variables. The wavevector k, defined as ##k = \frac{2\pi}{\lambda}##, is established as a fixed parameter in the equation, despite the existence of a spectrum of k values corresponding to different wave solutions. Participants clarify that while solutions can span multiple k values, each specific solution is derived for a singular, fixed k, leading to a set of solutions ##f_k## labeled by their respective wave numbers.

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fog37
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Hello Everyone,

Helmholtz equations derives from the wave equation by using separation of variables and assuming that the solution is indeed separable ##g(x,y,z,t) = f(x,y,z) T(t)##. The solutions to Helmholtz equations are functions of space, like f(x,y,z), and do not depend on time t.

the wavevector ##k = \frac{2\pi}{\lambda}## is present in the equation. Is that a constant or a variable? Solutions can span a spectrum of ##k## values so I don't believe the ##k## in the equation can be a constant otherwise the equation would be limited to function having a single and specific k value...

Thanks
 
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Different k values correspond to different waves with respect to wavelength or direction
 
True, but in the equation, is the k to be take as a variable?
 
Oh, that was your question. No, wavevector k is fixed.
 
I would say that the wave vector ##\mathbf{k}## is a parameter, since you solve the equation for fixed ##\mathbf{k}## but the value depend on the specific problem you want to solve.
 
so are you saying the solutions to this equation can only have a single k since the equation itself has a single k?
 
Presumably, this is a matter of convention. But, my personal point of view is the following (maybe other people on this forum will not agree). In your first post you are saying:
fog37 said:
Solutions can span a spectrum of ##k## values so I don't believe the ##k## in the equation can be a constant otherwise the equation would be limited to function having a single and specific k value...

We have therefore a set of solutions ##f_k## labeled by the wave number ##\mathbf{k}##. As, I said before you are then solving the equation for a fixed ##\mathbf{k}## and obtain one ##f_k##. You can then repeat this and solve for arbitrary number of values of ##k## depending on which solutions on the set you are interesting in.
 

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