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Original file line number | Diff line number | Diff line change |
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%physical constants | ||
clear all; | ||
close all; | ||
load 'conductive-receivers.mat'; | ||
c0 = 2.998e8; | ||
eta0 = 120*pi; | ||
mu0 = pi*4e-7; | ||
eps0 = 1e-9/(36*pi); | ||
%box dimensions | ||
width = 0.09; % 10cm | ||
height = width; | ||
length = width; | ||
%source parameters | ||
f0 = 3e9; | ||
tw = 1e-8/pi; | ||
t0 = 4*tw; | ||
%spatial discretization | ||
adipose = 10; | ||
tumor = 60; | ||
sigma = 1; | ||
epsr = tumor; | ||
w = 2 * pi * f0; | ||
k = (w/c0)*sqrt(epsr-1j*sigma/(w*eps0)); | ||
beta = real(k); | ||
c = w / beta; | ||
lambda = c/f0; | ||
dxmax = lambda / 10; | ||
dx = dxmax; | ||
dy = dx; | ||
dz = dx; | ||
nx = round(width/dx); | ||
ny = round(height/dy); | ||
nz = round(length/dz); | ||
% material | ||
f0 = 3e9; % GHz | ||
eps = ones(nx,ny,nz) * eps0 * adipose; | ||
sigma = ones(nx,ny,nz) * f0 * 1e-9 * 0.5 - 0.5; | ||
%temporal discretization | ||
dt = 0.95/(c*sqrt(dx^-2+dy^-2+dz^-2)); | ||
%EM field dimensions | ||
Hx = zeros(nx,ny,nz); | ||
Hy = zeros(nx,ny,nz); | ||
Hz = zeros(nx,ny,nz); | ||
Ex = zeros(nx,ny,nz); | ||
Ey = zeros(nx,ny,nz); | ||
Ez = zeros(nx,ny,nz); | ||
%iteration | ||
i = 0; | ||
for n=1:1:n_iter | ||
%magnetic field derivatives | ||
Hxy = diff(Hx,1,2); | ||
Hxz = diff(Hx,1,3); | ||
Hzx = diff(Hz,1,1); | ||
Hzy = diff(Hz,1,2); | ||
Hyx = diff(Hy,1,1); | ||
Hyz = diff(Hy,1,3); | ||
%electric field maxwell equations | ||
epsi = eps(:,2:end-1,2:nz-1); | ||
ksi = (dt * sigma(:,2:end-1,2:nz-1)) ./ ( 2 * epsi ); | ||
c2 = (1./(1+ksi)).*(dt./epsi); | ||
c1 = (1-ksi)./(1+ksi); | ||
Ex(:,2:end-1,2:end-1) = c1.*Ex(:,2:end-1,2:nz-1) - c2.*((1/dy)*Hzy(:,1:end-1,2:end-1) - (1/dz)*Hyz(:,2:ny-1,1:end-1)); | ||
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||
epsi = eps(2:end-1,:,2:end-1); | ||
ksi = (dt * sigma(2:end-1,:,2:end-1)) ./ ( 2 * epsi ); | ||
c2 = (1./(1+ksi)).*(dt./epsi); | ||
c1 = (1-ksi)./(1+ksi); | ||
Ey(2:end-1,:,2:end-1) = c1.*Ey(2:end-1,:,2:end-1) - c2.*((1/dz)*Hxz(2:end-1,:,1:end-1) - (1/dx)*Hzx(1:end-1,:,2:end-1)); | ||
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||
epsi = eps(2:end-1,2:end-1,:); | ||
ksi = (dt * sigma(2:end-1,2:end-1,:)) ./ ( 2 * epsi ); | ||
c2 = (1./(1+ksi)).*(dt./epsi); | ||
c1 = (1-ksi)./(1+ksi); | ||
Ez(2:end-1,2:end-1,:) = c1.*Ez(2:end-1,2:end-1,:) - c2.*((1/dx)*Hyx(1:end-1,2:end-1,:) - (1/dy)*Hxy(2:end-1,1:end-1,:)); | ||
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||
%TR sources | ||
for k=1:1:nrec | ||
Ez(recx, recdy * k, recz) = Ez(recx, recdy * k, recz) + rec(k, n); | ||
end | ||
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||
%electric field derivatives | ||
Exy = diff(Ex,1,2); | ||
Exz = diff(Ex,1,3); | ||
Ezx = diff(Ez,1,1); | ||
Ezy = diff(Ez,1,2); | ||
Eyx = diff(Ey,1,1); | ||
Eyz = diff(Ey,1,3); | ||
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||
%magnetic field maxwell equations | ||
Hx(:,1:end-1,1:end-1) = Hx(:,1:end-1,1:end-1) + (dt/(mu0*dy))*Ezy(:,:,1:end-1) - (dt/(mu0*dz))*Eyz(:,1:end-1,:); | ||
Hy(1:end-1,:,1:end-1) = Hy(1:end-1,:,1:end-1) + (dt/(mu0*dz))*Exz(1:end-1,:,:) - (dt/(mu0*dx))*Ezx(:,:,1:end-1); | ||
Hz(1:end-1,1:end-1,:) = Hz(1:end-1,1:end-1,:) + (dt/(mu0*dx))*Eyx(:,1:end-1,:) - (dt/(mu0*dy))*Exy(1:end-1,:,:); | ||
%display | ||
if (mod(i,5)==0) | ||
slice(:,:)=Ez(round(nx/2),:,:); | ||
pcolor(slice'); | ||
colorbar; | ||
drawnow | ||
end | ||
i = i+1; | ||
disp(i) | ||
end |
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