Proving $\int_{\mathbb{R}^3}\Delta G(x,y)dx=1$ with Gauss's Theorem

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In summary: So, applying Gauss's theorem we can find the integral $\int_{\mathbb{R}^3} \Delta{G(x,y)} dy$ quite easily.
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evinda
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Hello! (Wave)We have $G(x,y)=-\frac{1}{4 \pi} \frac{1}{||\overline{x}-\overline{y}||}$ for $x, y \in \mathbb{R}^3$.I want to show that $\int_{\mathbb{R}^3} \Delta{G(x,y)} dx= 1$.

It suffices to show that $\int_{\mathbb{R}^3} \Delta{G(x,0)} dx= 1$, since setting $\overline{x}=x-y$ we have $G(\overline{x},0)=G(x,y)$, right?

It holds that $\Delta G(x,y)=0$ for $x \neq y$, so $\int_{\mathbb{R}^3} \Delta{G(x,0)} dx= \int_{B(0,r)} \Delta{G(x,0)}$.

How can we apply Gauss's theorem in order to compute the above integral?
 
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evinda said:
Hello! (Wave)We have $G(x,y)=-\frac{1}{4 \pi} \frac{1}{||\overline{x}-\overline{y}||}$ for $x, y \in \mathbb{R}^3$.I want to show that $\int_{\mathbb{R}^3} \Delta{G(x,y)} dx= 1$.

It suffices to show that $\int_{\mathbb{R}^3} \Delta{G(x,0)} dx= 1$, since setting $\overline{x}=x-y$ we have $G(\overline{x},0)=G(x,y)$, right?

It holds that $\Delta G(x,y)=0$ for $x \neq y$, so $\int_{\mathbb{R}^3} \Delta{G(x,0)} dx= \int_{B(0,r)} \Delta{G(x,0)}$.

How can we apply Gauss's theorem in order to compute the above integral?

Hi evinda! (Smile)

What do $\overline x$ and $\overline y$ represent?
And what is $\Delta{G(x,y)}$, since he Laplacian operator $\Delta$ usually applies only to some $x \in \mathbb R^3$? (Wondering)

Anyway, I think we would have:
$$\int_{\mathbb{R}^3} \Delta{G(x,0)} \,dx
=\lim_{r\to\infty} \int_{B(0,r)} \Delta{G(x,0)} \,dx
=\lim_{r\to\infty} \int_{B(0,r)} \nabla \cdot \nabla {G(x,0)} \,dx
\overset{\text{Gauss}}=\lim_{r\to\infty} \oint_{\partial B(0,r)} \nabla {G(x,0)} \,dS \\
=\lim_{r\to\infty} \oint_{\partial B(0,r)} \nabla {-\frac {1}{4\pi r}} \,dS
=\lim_{r\to\infty} \oint_{\partial B(0,r)} {\frac {1}{4\pi r^2}}\,dS
=\lim_{r\to\infty} {\frac {1}{4\pi r^2}}\cdot 4\pi r^2 = \lim_{r\to\infty} 1 = 1
$$
(Thinking)
 

Related to Proving $\int_{\mathbb{R}^3}\Delta G(x,y)dx=1$ with Gauss's Theorem

1. What is Gauss's Theorem and how does it relate to proving the integral of $\Delta G(x,y)$ is equal to 1?

Gauss's Theorem, also known as the Divergence Theorem, is a mathematical tool used to relate the flux of a vector field through a closed surface to the divergence of that vector field at points inside the surface. In this case, we can use Gauss's Theorem to relate the flux of the gradient of $G(x,y)$ through a closed surface to the value of $G(x,y)$ at points inside the surface, ultimately leading to the proof that $\int_{\mathbb{R}^3}\Delta G(x,y)dx=1$.

2. What is the significance of proving the integral of $\Delta G(x,y)$ is equal to 1?

This proof is significant because it demonstrates the fundamental relationship between the divergence of a vector field and the flux of that field through a closed surface. It also has practical applications in physics and engineering, as it allows for the calculation of important quantities such as electric charge and mass distribution.

3. What assumptions are necessary for this proof to hold true?

In order for this proof to hold true, we must assume that $G(x,y)$ is a continuously differentiable function and that the surface enclosing the region over which we are integrating is a closed surface. Additionally, the vector field associated with $G(x,y)$ must also be well-behaved and satisfy certain conditions.

4. Can this proof be extended to higher dimensions?

Yes, this proof can be extended to higher dimensions. In fact, Gauss's Theorem is a generalization of Green's Theorem in two dimensions, and can be further extended to three or more dimensions. The main idea remains the same: relating the flux of a vector field to the divergence of that field at points inside a closed surface.

5. How is this proof relevant to other areas of mathematics and science?

This proof has wide-ranging applications in mathematics, physics, and engineering. It is used in fields such as fluid dynamics, electromagnetism, and heat transfer to calculate important quantities and solve differential equations. It also has connections to other important theorems, such as Stokes' Theorem and the Fundamental Theorem of Calculus.

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