Solve PDE Uxx+Uyy=-2 with Boundary Conditions

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The discussion revolves around solving the partial differential equation (PDE) Uxx + Uyy = -2 with specified boundary conditions. The approach involves recognizing that the equation is a Poisson equation due to the non-homogeneous term on the right-hand side. The strategy proposed includes finding a particular solution that satisfies the right-hand side and then adding solutions of the associated homogeneous Laplace equation to meet the boundary conditions. The use of separation of variables is suggested, with solutions expressed in terms of hyperbolic functions. The conversation indicates a gradual return to familiarity with PDEs and emphasizes the importance of satisfying boundary conditions in the solution process.
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.
 
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.
 
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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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