Initial & Boundary Value Problem-Fourier

In summary, the conversation discusses an initial and boundary value problem involving a Laplace equation in polar coordinates. The problem is expressed in the form $U_{\rho \rho}+\frac{1}{\rho^2}U_{\theta \theta}=0$ to accurately represent the geometry of the problem. The conversation also discusses finding solutions of the form $R(\rho)\Theta(\theta)$ and determining the constants $c_k$ to solve the problem.
  • #1
mathmari
Gold Member
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Hey! :eek:

We have the initial and boundary value problem $$u_{xx}(x,y)+u_{yy}(x,y)=0 , x^2+y^2<1 \\ u(x,y)=0 \\ u(1, \theta)=\sin{\theta}, 0< \theta< \pi$$

$$U_{\rho \rho}(\rho, \theta)+ \frac{1}{\rho^2} U_{\theta \theta}=0, 0< \rho<1, 0< \theta< \pi$$

We are looking for solutions of the form $R(\rho) \Theta(\theta)$

$R(\rho) \Theta(0)=0 \Rightarrow \Theta(0)=0\\ R(\rho) \Theta(\pi)=0 \Rightarrow \Theta(\pi)=0$

$R''(\rho) \Theta(\theta)+ \frac{1}{\rho^2} R(\rho) \Theta''(\theta)=0\\ \frac{\Theta''(\theta)}{\Theta(\theta)}=-\rho^2 \frac{R''(\rho)}{R(\rho)}=-\lambda $

$\Theta''(\theta)+ \lambda \Theta(\theta)=0 \\ \Theta(0)=\Theta(\pi)=0$$\rho^2 R''(\rho)-\lambda R(\rho)=0$

$\lambda_k=k^2$

$\Theta_k(\theta)=\sin{k \theta}$

$\rho^2 R_k''(\rho)-k^2 R_k(\rho)=0$

We are looking for a solution of the form $R(\rho)=\rho^m \Rightarrow m(m-1) \rho^m-k^2 \rho^m=0$

$m^2-m-k^2=0$

$\Delta=1+4k^2$

$m=\frac{1 \pm \sqrt{1+4k^2}}{2}$

For $m>0$, the solution is unbounded.

$R_k(\rho)=\rho^{\frac{1+ \sqrt{1+4k^2}}{2}}$

$U_k(\rho, \theta)=\rho^{\frac{1+ \sqrt{1+4k^2}}{2}} \sin{k \theta}$

$U(\rho, \theta)=\sum c_k $We determine $c_k$$U(1, \theta)=\sum_{k=1}^{\theta} c_k \sin{k \theta}=\sin{\theta}$

$c_1=1\\c_k=0, k=2, \dots$

$$$$

Why is the problem in polar coordinates $$U_{\rho \rho}+\frac{1}{\rho^2}U_{\theta \theta}=0$$ and not $$U_{\rho \rho}+\frac{1}{\rho}U_{\rho}+\frac{1}{\rho^2}U_{\rho \rho}=0$$ ??
 
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  • #2
Hello there!

The reason the problem is in the form $U_{\rho \rho}+\frac{1}{\rho^2}U_{\theta \theta}=0$ is because we are dealing with a Laplace equation in polar coordinates. In polar coordinates, the distance from the origin, $\rho$, is a key variable and is used to define the geometry of the problem. The term $\frac{1}{\rho^2}$ in the equation is known as the "scale factor" and is necessary to take into account the changing distance from the origin.

If we were to use the form $U_{\rho \rho}+\frac{1}{\rho}U_{\rho}+\frac{1}{\rho^2}U_{\rho \rho}=0$, we would be incorporating an extra term that does not accurately represent the geometry of the problem. This would lead to incorrect solutions and would not accurately describe the physical system.

I hope this helps clarify the use of polar coordinates in this problem. Let me know if you have any further questions.
 

FAQ: Initial & Boundary Value Problem-Fourier

What is an initial value problem in Fourier analysis?

An initial value problem in Fourier analysis is a type of differential equation where the initial conditions for the dependent variable are given at a specific starting point. The goal is to find a solution that satisfies both the equation and the initial conditions.

What is a boundary value problem in Fourier analysis?

A boundary value problem in Fourier analysis is a type of differential equation where the dependent variable is given at certain points along the boundary of the domain. The goal is to find a solution that satisfies both the equation and the boundary conditions.

How are initial and boundary value problems related in Fourier analysis?

Initial and boundary value problems are complementary in Fourier analysis. In some cases, a solution to a boundary value problem can be used to solve an initial value problem, and vice versa. They both involve finding a solution that satisfies certain conditions at specific points.

What is the importance of Fourier analysis in solving initial and boundary value problems?

Fourier analysis is a powerful mathematical tool that allows for the decomposition of complex functions into simpler trigonometric functions. This makes it easier to solve initial and boundary value problems, as the equations become more manageable and can be solved using familiar techniques.

Are there any real-world applications of initial and boundary value problems in Fourier analysis?

Yes, there are many real-world applications of initial and boundary value problems in Fourier analysis. Examples include heat transfer problems in engineering, predicting weather patterns in meteorology, and analyzing electrical circuits in physics. Additionally, Fourier analysis is also used in image and signal processing, as well as in music and sound engineering.

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