Can All Vector Fields Be Represented by the Vector Laplacian?

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Discussion Overview

The discussion revolves around whether all vector fields can be represented as the vector Laplacian of another vector field. Participants explore the implications of this idea in the context of vector calculus and the Poisson equation.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested

Main Points Raised

  • Some participants question the validity of the assertion that all vector fields can be expressed as the vector Laplacian of another vector field.
  • One participant references Helmholtz's Theorem as a basis for their belief in the assertion.
  • Another participant analyzes the mathematical implications, suggesting that if the equation holds, it must apply to each component of the vector field, leading to the conclusion that it relates to the Poisson equation.
  • It is proposed that the Poisson equation may have infinitely many solutions if boundary conditions are not specified.

Areas of Agreement / Disagreement

Participants express differing views on whether all vector fields can be represented in this manner, indicating that multiple competing perspectives exist without a consensus.

Contextual Notes

The discussion highlights potential limitations related to boundary conditions and the existence of solutions to the Poisson equation, which remain unresolved.

LucasGB
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Can all vector fields be described as the vector Laplacian of another vector field?
 
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Perhaps I should elaborate a little bit. The vector Laplacian is an operator which allows us to obtain a vector field B from a vector field A (B is the vector Laplacian of A). My question is: is it correct to say that ALL vector fields D can be though of as being the vector Laplacian of another vector field C?
 


why do you think this should be true?
 


Because I saw a proof of Helmholtz's Theorem where the guy assumed this was true.
 


Hi!

It's an intriguing problem you're posting over here :)

So, if I got it correctly, the question is, if for any given field F there exists a field B such that \vec F=\Delta\vec B

Well, this is a vector equation, so it has (assuming it really holds) to hold for every component, which implies:

F_i=\partial^2_l B_i for all i = 1,2,3, or put another way:

F_i=\Delta B_i which is the Poisson equation.

So you have to find out if the Poisson equation always has a solution. I checked in Wikipedia - it was not clearly stated, but it looks like the equation is indeed analytically solvable via Green's functions.
 


That's a very interesting breakdown of the problem. In fact, I think, and I could be wrong, that if we don't specify boundary conditions, there are infinitely many solutions to Poisson's equation.
 

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