Laplacian solution(page 2) to Jackson 1.5

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The discussion centers on the Laplacian solution to Jackson 1.5, specifically the equation \(\nabla^2 \left(\frac{1}{r}\right)=-4\pi\delta^3(\mathbf r)\). This identity is validated through distribution theory, where the Laplacian of \(\frac{1}{r}\) is shown to equal \(-4\pi\) times the value of a test function \(\phi\) at the origin. The derivation involves applying the Laplacian operator in a distributional sense, confirming the result through integration against smooth compactly supported functions.

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daudaudaudau
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Hi.

In http://www-personal.umich.edu/~pran/jackson/P505/p1s.pdf" solution(page 2) to Jackson 1.5 it is stated that

[tex]\nabla^2 \left(\frac{1}{r}\right)=-4\pi\delta^3(\mathbf r)[/tex].

But why is this true?

[tex]\nabla^2\left(\frac{1}{r}\right)=\frac{1}{r^2}\frac{d}{d r}\left(r^2\frac{d}{dr}\frac{1}{r}\right)=\frac{1}{r^2}\frac{d}{dr}(-1)[/tex]
 
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This equality is to be understood in the distributional sense. It should be read as:

[tex]\int \frac{\Delta \phi}{|x|}\, \mathrm{d}x = -4\pi \phi (0), \qquad \forall \phi \in C^{\infty}_c (\mathbf{R}^3)[/tex]

:)
 

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