Vector Laplacian: Scalar or Vector?

In summary, the value of Vector_Laplacian is a vector according to the page https://en.wikipedia.org/wiki/Vector_Laplacian, but it is a scalar according to the page https://en.wikipedia.org/wiki/D'Alembertian. The Laplacian operator applied to a vector in Cartesian coordinates is equal to the sum of the second partial derivatives of each component of the vector. This is clarified on the page https://en.wikipedia.org/wiki/Mathematical_descriptions_of_the_electromagnetic_field#Gauge_freedom.
  • #1

olgerm

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according to this page https://en.wikipedia.org/wiki/Vector_Laplacian value of Vector_Laplacian is vector, but according to this page https://en.wikipedia.org/wiki/D'Alembertian value of Vector_Laplacian is scalar

8a806b56e1a8af77aca1897fcd8ebf9c.png

Is on of these pages wrong or I misunderstand it?

I am asking because I want to know what does Δ2 equal to in this
1ad8dd4174eba9373c9235546a3264b8.png
and this
5020dc7c1608d709fcad4d7db1f19b50.png
equation on this https://en.wikipedia.org/wiki/Mathematical_descriptions_of_the_electromagnetic_field#Coulomb_gauge page.
 
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  • #2
The d'Alembertian is a differential operator. You can apply it to a scalar and get a scalar, or you can apply it to a vector and get a vector.
 
  • #3
So since magnetic potential A in this equation
1ad8dd4174eba9373c9235546a3264b8.png
is vector ##\nabla^2=(\sum_{i=1}^3(\frac{\partial^2 A}{\partial x_i*\partial x_1});\sum_{i=1}^3(\frac{\partial^2 A}{\partial x_i*\partial x_2});\sum_{i=1}^3(\frac{\partial^2 A}{\partial x_i*\partial x_3}))## not ##\nabla^2=\sum_{i=1}^3(\frac{\partial^2 A}{\partial x_i^2})##?
These are Cartesian coordinates.
 
  • #4
It is unclear what you intend to write with these expressions. In particular, it is unclear what you intend for ##A## to be (the vector, the vector components, etc). I strongly suggest that you do not write vectors on component form (x;y;z), but instead use basis vectors. This will make it much clearer what is intended.

The Laplace operator applied to a vector in Cartesian coordinates is such that the ##x## component of ##\nabla^2 \vec A## is equal to ##\nabla^2 A_x##, where ##A_x## is the ##x## component of ##\vec A##.
 
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  • #6
olgerm said:
A is vector-field. I am trying to find out what does ##\nabla^2 A##, on this Wikipedia page
https://en.wikipedia.org/wiki/Mathematical_descriptions_of_the_electromagnetic_field#Gauge_freedom , equal to.
Is it that ##(\nabla^2 A)_i=\frac{\partial^2 A_i}{\partial x_i^2}## or ##(\nabla^2 A)_j=\sum_{i=1}^3(\frac{\partial^2 A_i}{\partial x_i \cdot \partial x_j})## or ##\nabla^2 A=\sum_{i=1}^3(\frac{\partial^2 A_i}{\partial x_i^2})##?
Where ##A_i## is the ##i## component of ##\vec A##.
Neither, see my previous post.

Your first option is just one term in the sum, your second is grad(div(A)) and not the Laplacian of A, your third is a scalar.
 
  • #9
Orodruin said:
Yes. Although this is only valid in Cartesian coordinates.
Ok, thanks.
 

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