有没有三维的FDTD MATLAB代码,计算多介质电磁场
时间: 2024-03-24 07:37:30 浏览: 84
基于Matlab语言实现电磁场中的FDTD算法编程.pdf
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是的,以下是一个简单的三维FDTD Matlab代码,用于计算多介质中的电磁场分布:
```matlab
% FDTD simulation of a 3D waveguide with multiple dielectric materials
% Define simulation parameters
dx = 0.01; % spatial step size
dt = 0.001; % time step size
T = 1; % total simulation time
Lx = 1; % waveguide length
Ly = 0.5; % waveguide width
Lz = 0.2; % waveguide height
% Define material properties and regions
mu0 = 4*pi*10^-7; % permeability of free space
epsilon0 = 8.854e-12; % permittivity of free space
epsilonr1 = 2.5; % relative permittivity of region 1
epsilonr2 = 4.0; % relative permittivity of region 2
epsilonr3 = 6.0; % relative permittivity of region 3
mur = 1; % relative permeability of waveguide
region1 = [0.2 0.8 0.2 0.8 0.2 0.4]; % region 1 boundaries
region2 = [0.2 0.8 0.2 0.8 0.4 0.6]; % region 2 boundaries
region3 = [0.2 0.8 0.2 0.8 0.6 0.8]; % region 3 boundaries
% Calculate material constants
c = 1/sqrt(mu0*epsilon0); % speed of light in free space
epsilon1 = epsilonr1*epsilon0; % permittivity of region 1
epsilon2 = epsilonr2*epsilon0; % permittivity of region 2
epsilon3 = epsilonr3*epsilon0; % permittivity of region 3
mu = mur*mu0; % permeability of waveguide
% Calculate grid dimensions
Nx = round(Lx/dx);
Ny = round(Ly/dx);
Nz = round(Lz/dx);
% Initialize electric and magnetic fields
Ex = zeros(Nx,Ny,Nz);
Ey = zeros(Nx,Ny,Nz);
Ez = zeros(Nx,Ny,Nz);
Hx = zeros(Nx,Ny,Nz);
Hy = zeros(Nx,Ny,Nz);
Hz = zeros(Nx,Ny,Nz);
% Define source function
f = @(t) sin(2*pi*10*t);
% Main simulation loop
for n = 1:round(T/dt)
% Update electric fields
for i = 1:Nx
for j = 1:Ny
for k = 1:Nz-1
if k < round(region1(5)/dx)
epsilon = epsilon1;
elseif k < round(region2(5)/dx)
epsilon = epsilon2;
else
epsilon = epsilon3;
end
Ez(i,j,k) = Ez(i,j,k) + (dt/(dx*epsilon))*...
(Hy(i,j,k) - Hy(i-1,j,k) - Hx(i,j,k) + Hx(i,j-1,k));
end
end
end
for i = 1:Nx
for j = 1:Ny-1
for k = 1:Nz
if k < round(region1(5)/dx)
epsilon = epsilon1;
elseif k < round(region2(5)/dx)
epsilon = epsilon2;
else
epsilon = epsilon3;
end
Ex(i,j,k) = Ex(i,j,k) + (dt/(dx*epsilon))*...
(Hz(i,j,k) - Hz(i,j+1,k) - Hy(i,j,k) + Hy(i,j,k-1));
end
end
end
for i = 1:Nx-1
for j = 1:Ny
for k = 1:Nz
if k < round(region1(5)/dx)
epsilon = epsilon1;
elseif k < round(region2(5)/dx)
epsilon = epsilon2;
else
epsilon = epsilon3;
end
Ey(i,j,k) = Ey(i,j,k) + (dt/(dx*epsilon))*...
(Hx(i,j,k) - Hx(i,j,k-1) - Hz(i,j,k) + Hz(i+1,j,k));
end
end
end
% Apply source function
Ey(round(Nx/2),round(Ny/2),1) = Ey(round(Nx/2),round(Ny/2),1) + f(n*dt);
% Update magnetic fields
for i = 1:Nx-1
for j = 1:Ny-1
for k = 1:Nz-1
if k < round(region1(5)/dx)
mu = mur*mu0;
elseif k < round(region2(5)/dx)
mu = mur*mu0;
else
mu = mur*mu0;
end
Hz(i,j,k) = Hz(i,j,k) + (dt/(dx*mu))*...
(Ex(i,j,k) - Ex(i,j+1,k) + Ey(i+1,j,k) - Ey(i,j,k)) ;
Hx(i,j,k) = Hx(i,j,k) + (dt/(dx*mu))*...
(Ey(i,j,k+1) - Ey(i,j,k) - Ez(i,j+1,k) + Ez(i,j,k));
Hy(i,j,k) = Hy(i,j,k) + (dt/(dx*mu))*...
(Ez(i+1,j,k) - Ez(i,j,k) - Ex(i,j,k+1) + Ex(i,j,k));
end
end
end
% Plot electric field
imagesc(squeeze(Ex(:,:,round(Nz/2)))');
colormap(jet);
colorbar;
drawnow;
end
```
此代码使用了三维FDTD算法,通过在每个网格点处计算电场和磁场分量,并使用Maxwell方程组进行递推计算,得到电磁场的时变分布。在这个例子中,我们在波导中心的一个网格点处施加了一个10 Hz的正弦波形源,然后计算了电场的分布情况。此外,我们还定义了三个具有不同相对介电常数的区域,以模拟多介质情况。
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