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bitirme4.m
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bitirme4.m
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clear all
close all
%TMz Polarization
%physical constants
c = 2.998e8;
eta0 = 120*pi;
mu0 = pi*4e-7;
eps0 = 1e-9/(36*pi);
%environment parameters
nx = 249;
ny = 249;
delta = 1.2e-2; %1.2cm
dx = delta;
dy = delta;
dt = 20e-12; %0.95/(c*sqrt(dx^-2+dy^-2));
f0 = 2e9; %2GHz
tw = 16*dt;
t0 = 200*dt;
eps_r = 4.58;
sigma = 0.52; %S/m
ksi = (dt * sigma) / ( 2 * eps0* eps_r );
%calculation parameters
n_iter = 5000;
%initalization
Hx = zeros(nx,ny);
Hy = zeros(nx,ny);
Ez = zeros(nx,ny);
%iteration
for n=1:1:n_iter
%Maxwell Equations (TMz)
Ezx = diff(Ez,1,1);
Ezy = diff(Ez,1,2);
Hx(2:nx-1,2:ny) = Hx(2:nx-1,2:ny) - (dt/(mu0*dy))*Ezy(2:nx-1,:);
Hy(2:nx,2:ny-1) = Hy(2:nx,2:ny-1) + (dt/(mu0*dx))*Ezx(:,2:ny-1);
Hxy = diff(Hx,1,2);
Hyx = diff(Hy,1,1);
Ez(2:nx-1,2:ny-1) = ((1-ksi)/(1+ksi))*Ez(2:nx-1,2:ny-1) + ((1/(1+ksi))*(dt/(eps0*eps_r)))*((1/dx)*Hyx(2:nx-1,2:ny-1) - (1/dy)*Hxy(2:nx-1,2:ny-1));
%Gaussian Source
f(n)= sin(2*pi*f0*n*dt)*exp(-(n*dt-t0)^2/(tw^2))/dy;
Ez(round(nx/2),round(ny/2)) = Ez(round(nx/2),round(ny/2)) + f(n);
%Neuman Condition
Ez(:,2) = -Ez(:,1);
Ez(2,:) = -Ez(1,:);
Ez(:,ny-1) = -Ez(:,ny);
Ez(nx-1,:) = -Ez(nx,:);
%display
%n = n + 1;
pcolor(Ez);
shading interp;
drawnow
end