#PDE
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Have not done any work -
You could try two things here
First of all, if you denote L = (Δ + 100²), and the rhs f(x, y)
you want to find the following
- the solutions of Lu = 0
- a particular solution to Lu = -f
You may have a good shot if you look at stationary solutions in the form u(x, y) = v(x)w(y)
This was the also what I thought
Somehow I can use this to do Separation of variables
onto a Sturm Louiville System
@rustic bone
I dunno what that is
but if you have a solution for it, use it
Here I think in 2) you can get away with it with a little guess work
but in 1) it's a lot more complicated
According to wikipedia you solve it with separation of variables yes
Can you write it out?
$\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} + k^2 u = 0$
Rion
as we substitute
$\frac{d^2 v}{d x^2}(x) w(y) + v(x) \frac{d^2 w}{d y^2}(y) + k^2 v(x)w(y) = 0$
Rion
Somehow this is just screaming periodic functions
I found some solutions, which are as follows:
$v(x) = A_1\cos\left( \frac{k}{\sqrt{2}} x + \phi_1 \right)$
and
$w(y) = A_2\cos\left( \frac{k}{\sqrt{2}} y + \phi_2 \right)$
Or anything in their span I guess
Rion
However I don't really know how to show that we do not have any other plausible solution
which may not be true anyway
yeah but that's absolutely rigged
it doesn't exactly show that there is no other solution
that is not a combination of those
And it doesn't help our cause anyway, because we want to get a homogeneous equation solution
But in a sense I suppose that if we know that the above v and w will help construct a solution
then we'd want to look into sums of those solutions I suppose
$\sum_{i=0}^{\infty} a_j \cos\left( \frac{k}{\sqrt{2}} x + \phi_{1j} \right) \cos\left( \frac{k}{\sqrt{2}} y + \phi_{2j} \right)$
Rion
@sullen drum
This page gives you insights on how to find solutions for Lu = 0
just copy that shit
it's close enough to what i had in mind
hmm
For the particular solution you may want to try u(x, y) = v(x)w(y) with v and w quadratics wrt x and y
and you want to identify the coefficients
by expanding the rhs too
maybe that will work
Not sure I still get it
Well you see that the rhs is some sort of polynomial with x and y
So a plausible idea would be to look for polynomial particular solutions as well
Consider:
$u(x, y) = Kx(1-x) y(1-y) + \alpha y(1-y) + \beta x(1-x) + \alpha + \beta$
Rion
Then:
$\frac{\partial^2 u}{\partial x^2} (x, y) = -2Ky(1-y) - \beta$
Rion
And:
$\frac{\partial^2 u}{\partial y^2} (x, y) = -2Kx(1-x) - \alpha$
Rion
So:
$\frac{\partial^2 u}{\partial x^2} (x, y) + \frac{\partial^2 u}{\partial y^2} (x, y) + k^2 u(x, y) = k^2 Kx(1-x)y(1-y) + (\alpha - 2K)y(1-y) + (\beta-2K)x(1-x)$
Rion
Pick $\alpha = 2K$ and $\beta = 2K$ and then you've got yourself:
$\frac{\partial^2 u}{\partial x^2} (x, y) + \frac{\partial^2 u}{\partial y^2} (x, y) + k^2 u(x, y) = k^2 Kx(1-x)y(1-y)$
Rion
With k = 100² = 10^4, you just gotta choose K = -10² to get the result @sullen drum
That will get you a particular solution
But I haven't checked at all whether it fits the boundary conditions
$u(x, y) = K \left( x(1-x) y(1-y) + 2y(1-y) + 2x(1-x) + 4 \right)$
Rion
doesn't look like it though, maybe you need some additional term
or i guess adjust the homogeneous solution
Why
@rustic bone
I just fail to understand why we need to go through such a complicated method to find a particular solution
Or even how my particular solution is invalid
but I mean if that's what's expected of you then sure
Thank you @rustic bone +close