Dear Fellow Applied Physicists,
I have come across a simple problem turned complicated, where I attempt to solve a stationary 2D Laplace Equation (L.E) in order to better understand the effects of sharp edges on the solutions.
Starting from a simple setup, I solved, using a classic separation of variables technique, the L.E in 2D for a infinitely extended edge (with an opening angle of 120°) for the simple Dirichlet Boundary Condition of constant potential across the edge's infinite contour. The solution of this setup is easily found using 2D polar coordinates. However, once I add an additional geometric constraint to my problem, the Separation of Variables hypothesis no longer holds; thus I require some help here.
I have added one finite boundary to one of the edge's lengths, a finite value of length L, where this new boundary (at x = 0) behaves like a symmetry boundary condition.
The Laplace Equation (2 dimensional):
∇2 ϕ = 0
The boundary conditions in Cartesian coordinates are as follows:
1) ϕ = { V=const 0 < x < L & y = 0
L < x < +∞ & y = mx - mL for m = slope of boundary
}
2) ∇ ϕ|(x = 0 , y) = 0
I switched to Cartesian coordinates because the 2nd BC removes the separation of variables property when using polar coordinates, thus rendering it no more useful than a Cartesian formulation.
If you guys can, please either refer me to texts that tackle similar problems, or advise me on how to properly select solution methods for this problem. Separation of Variables doesn't work as far as I can tell, due to the BC.1 having y = f(x).
Please inform me if more details are needed.
Best,
Christopher