Solve PDE Uxx+Uyy=-2 with Boundary Conditions

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Homework Help Overview

The discussion revolves around solving the partial differential equation (PDE) Uxx + Uyy = -2, with specific boundary conditions. Participants are exploring methods to approach this problem, particularly focusing on the implications of the non-homogeneous term on the solution strategy.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Some participants discuss the possibility of solving the homogeneous part of the PDE and question whether this approach is appropriate given the presence of the non-homogeneous term. Others suggest finding a particular solution that satisfies the right-hand side and combining it with solutions of the homogeneous equation. There is mention of using separation of variables and the form of the solution involving eigenvalues.

Discussion Status

Participants are actively engaging with the problem, sharing their thoughts on potential methods and the nature of the PDE. Some have expressed uncertainty about their approaches, while others are considering the implications of boundary conditions on their solutions. There is a mix of exploration and clarification of concepts without a clear consensus on the best method yet.

Contextual Notes

Participants note the need to familiarize themselves with literature on inhomogeneous PDEs and the constraints posed by the boundary conditions. There is an acknowledgment of the complexity of the problem and the time required to work through it.

chwala
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Homework Statement
solve the inhomogenous pde below by considering the boundary conditions given
Relevant Equations
separation of variables.
1614169978889.png
ial

this is the question.
 
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its very long since i solved such questions during my post graduate class, i am trying to see if i can remember...
i attempted to solve the homogenous part, i just want to know if i am on the right track...
1614170283272.png

am i thinking right or i am missing something...from literature i can see that this does not qualify to be solved by the approach i have used of trying to solve homogenous pde...breaking them into ode. Since we have ##-2## on the rhs then it becomes poisson equation?
 
Last edited:
As with any linear problem the answer is "take something which satisfies the RHS and add something from the kernel".

So here: Find a function of (x,y) which satisfies \nabla^2 f = -2 and add solutions of Laplace's equation to satisfy the boundary condition. This is easier if your particular solution satisfies as much of the boundary condition as possible. Here I think you have less work if your function vanishes on x = 0 and x = 1.

Here you have u(x,0) = u(x,1) = u(1,-x) = -\sinh \pi \sin(\pi x).

Don't forget that you can use \cosh (kx) and \sinh(kx) in place of e^{\pm kx} and that \sinh(k(1 - x)) is a linear combination of these.
 
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I should be able to look at this during december...i have had too much work on my desk... and at same time need to familiarise with literature on inhomegenous pde's...
 
* Am on this now...allow me to deal with it slowly...am now conversant with pde's. This is Laplace equation...steady-state equation (Equilibrium solution).

We shall solve this by separation of variables, we shall seek solutions of the form:

##U(x,y) = X(x) Y(y)##

For the Homogenous part we shall have;

##X^{''}(x) Y(y) + X(x) Y^{''} (y) = 0##

it follows that,

##\dfrac{X^{''}(x)}{X(x)} = -\dfrac{Y^{''}(y)}{Y(y)} =±μ^2##

case 1; using eigenvalue ##[λ=μ^2]##

##X^{''} -μ^2X=0##
##Y^{''}+μ^2Y=0##

##X^{''} -μ^2X=0##

it follows that

##m^2-μ^2=0## is our characteristic equation, solving we get;

##m^2=μ^2##

##⇒m=\sqrt{μ^2}=μ## our solution would therefore be of the form;

##X=e^{μx}=A \cosh μx +B \sinh μx##

##X=A \cosh μx +B \sinh μx##

...will continue later.
 
Last edited:
Solution
<br /> u(x,y) = x(1-x) - \sum_{n=1}^\infty Y_n(y) a_n \sin (n \pi x) + \sinh(\pi x)\sin(\pi y) <br /> - ( \sinh (\pi y) + \sinh (\pi(1 - y)) )\sin (\pi x) where <br /> Y_n(y) = \frac{\sinh(n\pi y) + \sinh(n\pi(1-y))}{\sinh (n \pi)}<br /> is chosen such that Y_n(0) = Y_n(1) = 1 and <br /> \sum_{n=1}^\infty a_n \sin (n \pi x) = x(1-x).
 
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