Proving Laplace Equation in $\Omega_{(a,b)}$

In summary: Therefore, by the continuity of composition, $v$ must have a continuous derivate in $\Omega_{(a,b)}$.
  • #1
Julio1
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Let $\Omega$ an open domain in $\mathbb{R}^2.$ Suppose that $u$ is an application $C^2$ that satisfy the Laplace equation $\Delta u=0$ in $\Omega.$ Let $\Omega_{(a,b)}=\{(x+a,y+b): (x,y)\in \Omega\}$ and define $v(X,Y)=u(X-a,Y-b)$ for all $(X,Y)\in \Omega_{(a,b)}.$ Show that $v$ is an application $C^2$ on $\Omega_{(a,b)}$ and satisfy the equation $\dfrac{\partial^2 v}{\partial X^2}+\dfrac{\partial^2 v}{\partial Y^2}=0$ in $\Omega_{(a,b)}.$

Hello MHB :). My question is, can use Chain Rule for this case? and how or that form can be used?
 
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  • #2
Can someone help me out?
 
  • #3
Hi Julio,

Let $x = X-a$ and $y=Y-b$, so that $v(X,Y)=u(x,y)$. Since $v$ is the composition of $u$ with the translation map $(X,Y) \mapsto (X-a,Y-b)$ and $u$ is $C^2$ in $\Omega$, then $v$ is $C^2$ in $\Omega_{(a,b)}$. By the chain rule, argue that $$\frac{\partial^2 v} {\partial X^2} + \frac{\partial^2 v}{\partial Y^2} = \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0.$$
 
  • #4
Euge said:
Hi Julio,

Let $x = X-a$ and $y=Y-b$, so that $v(X,Y)=u(x,y)$. Since $v$ is the composition of $u$ with the translation map $(X,Y) \mapsto (X-a,Y-b)$ and $u$ is $C^2$ in $\Omega$, then $v$ is $C^2$ in $\Omega_{(a,b)}$. By the chain rule, argue that $$\frac{\partial^2 v} {\partial X^2} + \frac{\partial^2 v}{\partial Y^2} = \frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} = 0.$$

Thanks Euge :).

But for show that $v\in C^2(\Omega_{(a,b)})$ I don't can show that $v$ has continuous derivate? It is necessary for this case?
 
  • #5
Can help me? :(
 
  • #6
Julio, please do not bump threads. Since $v$ is the composition of $C^2$ maps (i.e., the map $u$ and the translation map $(X,Y) \mapsto (X-a,Y-b)$), it is $C^2$.
 

Related to Proving Laplace Equation in $\Omega_{(a,b)}$

What is the Laplace Equation and where is it used?

The Laplace Equation is a partial differential equation that describes the distribution of a scalar quantity, such as temperature or pressure, in a given region. It is used in many areas of science and engineering, including fluid mechanics, electromagnetism, and heat transfer.

What is the domain and range of the Laplace Equation?

The domain of the Laplace Equation is typically a bounded region in space, denoted by Ω. The range of the equation is the set of all possible solutions, which are scalar fields that satisfy the given boundary conditions.

What is the significance of the Laplace Equation in mathematics?

The Laplace Equation is a fundamental equation in mathematics and has many important applications, such as in potential theory and harmonic analysis. It also serves as a building block for more complex equations and has connections to other areas of mathematics, such as complex analysis and Fourier analysis.

What are the boundary conditions for solving the Laplace Equation?

The boundary conditions for solving the Laplace Equation depend on the specific problem at hand. They typically include specifying the values of the scalar field at the boundary of the domain Ω, as well as any necessary derivatives of the field. These conditions are necessary for finding a unique solution to the equation.

How can the Laplace Equation be proven in a bounded region Ω?

The Laplace Equation can be proven in a bounded region Ω using various techniques, such as separation of variables, Green's functions, and conformal mapping. These methods involve manipulating the equation and applying mathematical concepts to arrive at a solution that satisfies the given boundary conditions. Each approach has its own advantages and limitations, and the choice of method depends on the specific problem being solved.

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