Coming from engineering rather than mathematics, I am recently dealing with non-linear partial differential equations e.g. like the well known Korteweg-de-Vries equation:
$$u_{t} + uu_x + u_{xxx} = 0$$
In the literature I found the two- and three-dimensional versions of the KdV-equation:
$$(u_{t} + uu_x + u_{xxx})_x + u_{yy} = 0 $$ $$(u_{t} + uu_x + u_{xxx})_x + u_{yy} + u_{zz} = 0$$
What bugs me now is how one derives the two- respectively three-dimensional versions from the original version? In all of the literature I have found so far, the multi-dimensional version seems to fall from heaven, nowhere I could find a complete derivation or any intuition behind it. This is unfortunately not the first time I can not grasp how one author jumps from the 1-D to a n-D version.
So generally asked: How does one derive a multi-dimensional version of a (non-linear)PDE given a 1 + time-dimensional form like the first equation? It would be more clear to me if the original version would be written in vector notation (with $\nabla$, $\cdot$, $\times$, $\Delta$, etc. operators). Would be great if someone with a more profound mathematical background could educate me.
Thanks a lot!
Edit:
The 2D version is also called Kadomtsev-Petviashvili equation, if that rings a bell for anyone.
I'm not sure how one would derive the analog, but my gut feeling is that one would generalize the KdV hamiltonian (which is the second (aka "energy") integral of motion on the wikipedia page). I'm not sure if Hamiltonian mechanics is something you've covered in engineering courses, as it can quickly turn into very advanced/technical pure mathematics, but the legend Jerrold Marsden was an absolute pioneer of not only developing this advanced pure math, but also applying it to real engineering problems (he was a Professor of Engineering and Control & Dynamical Systems at CalTech). There is a great lecture of his on YouTube that highlights applications of his research to problems in engineering.
There is a "2D analog" of KdV, it's called the "Kadomtsev–Petviashvili Equation" (KP). Like KdV, it is integrable (it has countably infinitely many conserved quantities/integrals of motion). I wonder if you took the Hamiltonian for the KP equation and only kept one spatial dimension, if it would be equal to the KdV Hamiltonian. Perhaps I shall try it!