Poisson's Formula for the half space

  • Thread starter Thread starter docnet
  • Start date Start date
  • Tags Tags
    Formula Space
Click For Summary
SUMMARY

The discussion focuses on Poisson's Formula for the half space, specifically the application of Green's functions in the context of the Laplace equation in \( R^3_+ \). The key components include the mapping of points via the reflection operator \( \Lambda(x_1,x_2,x_3)=(x_1,x_2,-x_3) \) and the fundamental solution \( \Phi=\frac{1}{4\pi ||x||} \). The derived Green's function is expressed as \( G(x,y)=\frac{1}{4\pi ||y-x||}-\frac{1}{4\pi ||y-\bar{x}||} \), and the outward-pointing unit normal vector field is defined on the boundary \( \{x_3=0\} \) as \( \nu=-\vec{e}_3 \). The discussion seeks feedback on the correctness of these formulations and the next steps in the analysis.

PREREQUISITES
  • Understanding of Green's functions in partial differential equations
  • Familiarity with Laplace's equation and boundary value problems
  • Knowledge of vector calculus, particularly normal vector fields
  • Proficiency in mathematical notation and operations in \( R^n \)
NEXT STEPS
  • Explore the derivation and applications of Green's functions in various boundary conditions
  • Study the implications of reflection operators in higher-dimensional spaces
  • Investigate the properties of the Laplace operator in half-space domains
  • Learn about the numerical methods for solving boundary value problems in \( R^3_+ \)
USEFUL FOR

Mathematicians, physicists, and engineers working with partial differential equations, particularly those focusing on boundary value problems and Green's function methodologies.

docnet
Messages
796
Reaction score
486
Homework Statement
psb
Relevant Equations
psb
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?
 
Physics news on Phys.org
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
$$\frac{\partial }{\partial (-\vec{e}_3)}G(x,y)\Rightarrow \frac{1}{4\pi}\frac{\partial }{\partial (-\vec{e}_3)}\Big[\frac{1}{ ||y-x||}-\frac{1}{||y-\bar{x}||}\Big]$$
 

Similar threads

  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 7 ·
Replies
7
Views
2K
Replies
3
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 11 ·
Replies
11
Views
3K
Replies
10
Views
3K
Replies
12
Views
2K
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K