InversePDE / data /eit-data /matlab-code /BoundaryData.m
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% 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