Function whose 2nd order divergence is the Dirac Delta

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SUMMARY

The discussion focuses on the derivation and uniqueness of the Green's function G for the Poisson's equation, specifically addressing the equation \nabla^2 \cdot G(\textbf{r}, \textbf{r}') = \delta(\textbf{r}-\textbf{r}'). The proposed solution is G(\textbf{r}, \textbf{r}') = -\frac{1}{4\pi}\frac{1}{|\textbf{r} - \textbf{r}'|}, which satisfies the equation under the condition that |G| approaches 0 as |\textbf{r}| approaches 0. However, the uniqueness of this solution is questioned, with the acknowledgment that the general form of the Green's function may include an additional term F(r,r') that satisfies \nabla^2F(r,r') = 0, depending on boundary conditions.

PREREQUISITES
  • Understanding of Poisson's equation and its applications.
  • Familiarity with Green's functions in the context of differential equations.
  • Knowledge of vector calculus, particularly the divergence operator.
  • Basic concepts of boundary conditions in mathematical physics.
NEXT STEPS
  • Study the derivation of Green's functions for various boundary conditions.
  • Learn about the uniqueness theorem for solutions to partial differential equations.
  • Explore the implications of the Laplace operator in different coordinate systems.
  • Investigate the role of singularities in the context of Green's functions.
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Mathematicians, physicists, and engineering students who are studying differential equations, particularly those interested in the applications of Green's functions in solving boundary value problems.

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Homework Statement



This problem came when I was learning the Poisson's equation (refer to http://farside.ph.utexas.edu/teaching/em/lectures/node31.html). when it came to the step to find the Green's function G which satisfies \nabla^2 \cdot G(\textbf{r}, \textbf{r}') = \delta(\textbf{r}-\textbf{r}') with |G| \rightarrow 0 when |\textbf{r}| \rightarrow 0, the tutorial I refer to simply yields G(\textbf{r}, \textbf{r}') = -\frac{1}{4\pi}\frac{1}{|\textbf{r} - \textbf{r}'|}.

I understand that \int_{V} \nabla^2 \cdot \frac{1}{|\textbf{r} - \textbf{r}'|} dV= \int_{S=\partial V} \nabla \cdot \frac{1}{|\textbf{r}-\textbf{r}'|} \cdot d\textbf{S} = \int_{S=\partial V} -\frac{\textbf{r}-\textbf{r}'}{|\textbf{r}-\textbf{r}'|^3} \cdot d\textbf{S} = -4\pi, by assuming that V is a unit sphere located at \textbf{r}'. Thus G(\textbf{r}, \textbf{r}') = -\frac{1}{4\pi}\frac{1}{|\textbf{r} - \textbf{r}'|} COULD BE ONE SOLUTION to the equation, but what about proof of the uniqueness? Is this the only solution to the equation \nabla^2 \cdot G(\textbf{r}, \textbf{r}') = \delta(\textbf{r}-\textbf{r}') with |G| \rightarrow 0 when |\textbf{r}| \rightarrow 0?

Homework Equations



\textbf{r} = x \cdot \textbf{i} + y \cdot \textbf{j} + z \cdot \textbf{k}
\textbf{r}' = x' \cdot \textbf{i} + y' \cdot \textbf{j} + z' \cdot \textbf{k}
\nabla = \frac{\partial}{\partial x} \cdot \textbf{i} + \frac{\partial}{\partial y} \cdot \textbf{j} + \frac{\partial}{\partial z} \cdot \textbf{k}
\delta(\textbf{r}) = \delta(x) \cdot \delta(y) \cdot \delta(z)

The Attempt at a Solution



Stated above.
 
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From what I recall the Green's function of the Laplace operator is not unique, and it's most general form would be ##G(r,r ′ )=−\frac{1}{4\pi}\frac{1}{|r−r ′|} + F(r,r')## such that ##F(r,r')## satisfies ##\nabla^2F(r,r') = 0##. Depending on the type of boundary conditions, symmetry, etc, ##F(r,r')## can be chosen to simplify the problem. I'm pretty rusty with my Green's functions though so if I'm mistaken someone please correct me.
 
@Miles, yes you are right that the general equation is not guaranteed a unique solution. However I am bad at differential equations such that even given the boundary condition |G| \rightarrow \infty when |\textbf{r}| \rightarrow 0, I can't figure out the answer to my question :(
 

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