I am used to solving elliptic PDEs of even order. I was wondering what would one do for odd order PDEs. Notably the discretisations of those results in unsymmetric matrices. I tried solving the following simple problem:
$$\frac{d^3u}{dx^3}(x) = 0,\, x\in \Omega \quad u(x) = f(x), \, x \in \Gamma_D, \, \partial^{l}_nu(x) = 0, x\in\Gamma_N$$
I would generally expect to get some quadratic spline as the solution to the above. But I got a very oscillatory solution which I believe is due to numerical instability. I used the discretisation: $$\frac{d^3u}{dx^3} = \begin{bmatrix} -\frac{1}{2} & 1 & 0 & -1 & \frac{1}{2} \end{bmatrix} *u+O(h^2)$$
Since the system matrix $L$ is unsymmetric, I use a CGNR solver to solve $L^TLx = L^Tb$ instead, but nevertheless things don't seem to work out. I have never dealt with odd-order PDEs numerically. Are there some references discussing this? Am I supposed to use a specific discretisation like an upwind scheme? I don't think this makes any sense as the factor in front of $\frac{d^3u}{dx^3}$ seems to be irrelevant considering that the right-hand side is zero. Would the above problem be stabilized by solving:
$$\left |\frac{d^3u}{dx^3}\right | = 0,$$
instead? Clearly I cannot write the above as $y=Lx$ anymore and would have to potentially extend it to $\partial_t u = \left|\frac{d^3u}{dx^3}\right|$, e.g. apply explicit Euler and send the time to infinity. I just want to make sure whether there are known methods to handle odd order PDEs numerically before I try some stupid ideas.