Poisson's Formula for the half space

In summary, we discussed the map ##\Lambda## that takes a point ##x## in the set ##R^n\backslash \{0\}## into the reflected point ##\bar{x}## in the set ##R^n\backslash R^3_+##. We also introduced the fundamental solution ##\Phi## and the green's function ##G(x,y)## for the problem $$\Delta u=f$$ in ##R^3_+## with boundary condition ##u=g## on ##\partial R^3_+##. We then showed the outward-pointing unit normal vector field on the boundary and how to compute the derivative of ##G(x,y)## in the direction of this vector field
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Hi all, thanks in advance for any constructive feedback. :bow:

Screen Shot 2021-03-05 at 11.22.59 PM.png
Screen Shot 2021-03-05 at 11.23.04 PM.png


Definition:
If ##x\in R^n\backslash \{0\}## then the map ##\Lambda## takes the point ##x## into ##\bar{x}\in R^n\backslash R^+_3## given by ##\bar{x}=\{x_1,x_2,-x_3\}##

We take the reflected point ##\bar{x}## and the fundamental solution
$$\Phi=\frac{1}{4\pi ||x||}$$ then
$$\phi^x(y)=\frac{1}{4\pi ||y-\bar{x}||}$$
and hence $$G(x,y)=\frac{1}{4\pi ||y-x||}-\frac{1}{4\pi ||y-\bar{x}||}$$ is the green's function for ##R^+_3##

The outward pointing unit normal vector field on the boundary is given by a function ##\nu## that assigns a unit vector ##-\vec{e}_3## to every point on ##x_3=0##.

The differential operator $$\frac{\partial}{\partial \nu}\rightarrow\frac{-\partial }{\partial x_3}$$

The derivative of ##G(x,y)## in the direction of the vector field ##\nu## is given by
$$\frac{\partial }{\partial \nu}G(x,y)= \frac{-\partial }{\partial x_3}\Big[\Phi (y-x)-\Phi(y-\bar{x})\Big]=\frac{-\partial }{\partial x_3}\Big[\frac{1}{4\pi ||y-x||}-\frac{1}{4\pi ||y-\bar{x}||}\Big]$$

Have I made mistakes so far, and can I continue working?
 
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update with "progress"

Definition:
If ##x\in R^n\backslash \{0\}##, then the map $$\Lambda(x_1,x_2,x_3)=(x_1,x_2,-x_3)$$ takes every point ##x## into ##\bar{x}=\{x_1,x_2,-x_3\}\in R^n\backslash R^3_+##

To solve the problem
$$
\begin{cases}
& \Delta u=f \quad \text{in} \quad R^3_+\\
& u= g \quad \text{on} \quad \partial R^3_+
\end{cases}
$$
We consider the reflected point ##\bar{x}## and the fundamental solution ##\Phi=\frac{1}{4\pi ||x||}##. The following problem
$$
\begin{cases}
& \Delta \phi^x=0 \quad \text{in} \quad R^3_+\\
& \phi^x(y)= \Phi(y-x) \quad \text{on} \quad \partial R^3_+
\end{cases}
$$
gives the corrector function
$$\phi^x(y)=\frac{1}{4\pi ||y-\bar{x}||}$$
and hence the green's function is $$G(x,y)=\frac{1}{4\pi ||y-x||}-\frac{1}{4\pi ||y-\bar{x}||}$$
The outward-pointing unit normal vector field on the set ##\{x_3=0\}## is given by a function ##\nu## that assigns the unit vector ##-\vec{e}_3## to every point on the set ##\{x_3=0\}##. Let us take the differential operator $$\frac{\partial}{\partial \nu}\Rightarrow\frac{\partial }{\partial (-\vec{e}_3)}$$
and compute the derivative of ##G(x,y)## in the direction ##\nu## on the set ##\{x_3=0\}## in the flat Euclidean connection
$$\frac{\partial }{\partial (-\vec{e}_3)}G(x,y)\Rightarrow \frac{1}{4\pi}\frac{\partial }{\partial (-\vec{e}_3)}\Big[\frac{1}{ ||y-x||}-\frac{1}{||y-\bar{x}||}\Big]$$
 

1. What is Poisson's Formula for the half space?

Poisson's Formula for the half space is a mathematical formula that relates the behavior of a harmonic function on the boundary of a half space to its behavior inside the half space. It is a fundamental tool in the study of partial differential equations.

2. How is Poisson's Formula derived?

Poisson's Formula is derived using the method of images, which involves creating a "mirror image" of the original boundary function and using it to solve the problem. This technique is based on the principle of superposition, where the solution to a problem is the sum of individual solutions to simpler problems.

3. What are the applications of Poisson's Formula for the half space?

Poisson's Formula has a wide range of applications in physics, engineering, and other fields. It is commonly used to solve problems in electrostatics, heat conduction, fluid mechanics, and potential theory. It is also a useful tool in solving boundary value problems for partial differential equations.

4. Can Poisson's Formula be extended to higher dimensions?

Yes, Poisson's Formula can be extended to higher dimensions, such as the full space or a general domain. However, the method of images is not applicable in higher dimensions, and other techniques must be used to derive the formula.

5. Are there any limitations to using Poisson's Formula for the half space?

While Poisson's Formula is a powerful tool for solving boundary value problems, it does have some limitations. It can only be applied to linear problems, and the boundary conditions must be specified on a flat boundary. It also assumes that the solution is continuous and differentiable inside the half space.

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