| % Description of Neumann boundary condition for the | |
| % conductivity problem. | |
| % | |
| % The format of this file is suitable for describing the boundary condition | |
| % for the assempde.m routine of Matlabs PDE toolbox. | |
| % | |
| % Arguments: | |
| % p triangulation points | |
| % e edge data | |
| % u not used here | |
| % time not used here | |
| % | |
| % Returns: | |
| % q zeros(1,ne), where ne is the number of edges in e | |
| % g values of Neumann data at centerpoint on each edge | |
| % h ones(1,2*ne) | |
| % r zeros(1,2*ne) | |
| % | |
| % Samuli Siltanen May 2008 | |
| function [q,g,h,r] = BoundaryData(p,e,u,time) | |
| % Number of edges | |
| ne = size(e,2); | |
| % Give value to q, g and h | |
| q = zeros(1,ne); | |
| h = zeros(1,2*ne); | |
| r = zeros(1,2*ne); | |
| % Initialize Neumann data matrix | |
| g = zeros(1,ne); | |
| % Initialize vector for storing edge lengths for integration | |
| elen = zeros(1,ne); | |
| % Loop over edges | |
| for nnn = 1:ne | |
| % Coordinates of starting and ending points of the current edge | |
| sp1 = p(1,e(1,nnn)); | |
| sp2 = p(2,e(1,nnn)); | |
| ep1 = p(1,e(2,nnn)); | |
| ep2 = p(2,e(2,nnn)); | |
| % Compute midpoint of boundary segment | |
| mp1 = (sp1+ep1)/2; | |
| mp2 = (sp2+ep2)/2; | |
| % Record length of edge | |
| elen(nnn) = abs((sp1+i*sp2)-(mp1+i*mp2)); | |
| % Evaluate Neumann data at the plane point (mp1,mp2) | |
| % We know that this trigonometric data integrates to zero, | |
| % ensuring solvability of the Neumann problem. | |
| load data/BoundaryDataN n | |
| g(nnn) = 1/sqrt(2*pi)*exp(i*n*angle(mp1+i*mp2)); | |
| end | |