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时域有限差分法 FDTD
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我们一起来讨论1D FDTD (附代码)
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我们一起来讨论1D FDTD (附代码)
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opticalboy
UID :13713
注册:
2008-06-12
登录:
2008-07-11
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仿真新人
0楼
发表于: 2008-06-17 11:50:16
%***********************************************************************
RG45S0Ygj
% 1-D FDTD code with simple radiation boundary conditions
(}X5*BB&
%***********************************************************************
a8T9=KY^
%
_)5E=
% Program author: Susan C. Hagness
<Y"RsW9
% Department of Electrical and Computer Engineering
A Qjv? 4)T
% University of Wisconsin-Madison
q$"u<
% 1415 Engineering Drive
-rcEG!
% Madison, WI 53706-1691
; j.d
% 608-265-5739
bDWLHdu a
%
hagness@engr.wisc.edu
jnp~ACN,
%
4utwcXL
% Date of this version: February 2000
}V]b4t
%
o i'iZX
% This MATLAB M-file implements the finite-difference time-domain
;?HP/dZLz
% solution of Maxwell's curl equations over a one-dimensional space
K]$PRg1|3
% lattice comprised of uniform grid cells.
k5-4^
%
OlyW/hd
% To illustrate the algorithm, a sinusoidal wave (1GHz) propagating
p}pRf@(`\
% in a nonpermeable lossy medium (epsr=1.0, sigma=5.0e-3 S/m) is
<MG&3L.[
% modeled. The simplified finite difference system for nonpermeable
pl r@
% media (discussed in Section 3.6.6 of the text) is implemented.
Fya*[)HBo
%
n! 5(Z5=
% The grid resolution (dx = 1.5 cm) is chosen to provide 20
I=&i &6v8G
% samples per wavelength. The Courant factor S=c*dt/dx is set to
m@kLZimD
% the stability limit: S=1. In 1-D, this is the "magic time step."
ddN(L`nd
%
y_L8i[
% The computational domain is truncated using the simplest radiation
#^VZJ:2=|
% boundary condition for wave propagation in free space:
E}9wzPs
%
CJN~p]\
% Ez(imax,n+1) = Ez(imax-1,n)
*bp09XG
%
*D%w r'!>
% To execute this M-file, type "fdtd1D" at the MATLAB prompt.
k vZ w4Pk
% This M-file displays the FDTD-computed Ez and Hy fields at every
*ilh/Hd>
% time step, and records those frames in a movie matrix, M, which is
| I:@:
% played at the end of the simulation using the "movie" command.
L3\#ufytb
%
'-A;B.GV%
%***********************************************************************
Vc5>I_
m BvO<?ec
clear
w3q'n%
FLG"c690
%***********************************************************************
T=YVG@fm?
% Fundamental constants
0e0)1;t\
%***********************************************************************
!aUYidd
=M-=94
cc=2.99792458e8; %speed of light in free space
$Z)u04;&@
muz=4.0*pi*1.0e-7; %permeability of free space
+r"}@8/\1
epsz=1.0/(cc*cc*muz); %permittivity of free space
-B-G$ii
rtAPkXJFM
freq=1.0e+9; %frequency of source excitation
f$:Y'$Z1
lambda=cc/freq; %wavelength of source excitation
TsT5BC63
omega=2.0*pi*freq;
mmJnE
M *w{PjU
%***********************************************************************
PY_8*~Z
% Grid parameters
?`e@ o?
%***********************************************************************
^X{U7?x
#%QHb,lhl
ie=200; %number of grid cells in x-direction
d`rZgY
9NwUXh(:(
ib=ie+1;
j"6|$Ze8
U%bm{oVn
dx=lambda/20.0; %space increment of 1-D lattice
.g}N@
dt=dx/cc; %time step
)e5=<'f1
omegadt=omega*dt;
P6kDtUXF
IH=$ wc
nmax=round(12.0e-9/dt); %total number of time steps
*7H *epUa
$=diG
%***********************************************************************
plPPf+\
% Material parameters
'|=Pw
%***********************************************************************
4o M~
AJ6l#j-
eps=1.0;
rM.Pc?Z
sig=5.0e-3;
^k7I+A
@4UX~=:686
%***********************************************************************
;MNUT,U
% Updating coefficients for space region with nonpermeable media
(U#,;
%***********************************************************************
PP$2s]{
&c!6e<o[p
scfact=dt/muz/dx;
%ZD]qaU0
W8bp3JX"
ca=(1.0-(dt*sig)/(2.0*epsz*eps))/(1.0+(dt*sig)/(2.0*epsz*eps));
?3K~4-!?/
cb=scfact*(dt/epsz/eps/dx)/(1.0+(dt*sig)/(2.0*epsz*eps));
$\*Z
Mm*V;ADF
%***********************************************************************
OWrQKd
% Field arrays
<eMqg u
%***********************************************************************
l4i51S"
IrZ\;!NK
ez(1:ib)=0.0;
ds+K7B$
hy(1:ie)=0.0;
I,#E`)
@yb'h`f]
%***********************************************************************
@` Pn<_L
% Movie initialization
?jfh'mCA
%***********************************************************************
]Xa]a}[uE
E8Kk)7
x=linspace(dx,ie*dx,ie);
sE&nEc
{sB-"NR`K
subplot(2,1,1),plot(x,ez(1:ie)/scfact,'r'),axis([0 3 -1 1]);
d+)L K~
ylabel('EZ');
VRY(@# q
e@VJ-s
subplot(2,1,2),plot(x,hy,'b'),axis([0 3 -3.0e-3 3.0e-3]);
USEmD5 q
xlabel('x (meters)');ylabel('HY');
U@).jpN
6_" n
rect=get(gcf,'Position');
qspGNu
rect(1:2)=[0 0];
0vLx={i
pSC{0Y$g
M=moviein(nmax/2,gcf,rect);
V0m1>{
EsWB |V>
%***********************************************************************
@F(er
% BEGIN TIME-STEPPING LOOP
`:Wyw<^
%***********************************************************************
bE% Hm!
/Z*$k{qIR&
for n=1:nmax
;p*L(8<YI
6[XaIco=C
%***********************************************************************
A4l"^dZc
% Update electric fields
b/*QV0(
%***********************************************************************
,B;mG]_
mQ}\ptdfV
ez(1)=scfact*sin(omegadt*n);
PT,*KYF_O"
jN{k }
rbc=ez(ie);
+e>G V61
ez(2:ie)=ca*ez(2:ie)+cb*(hy(2:ie)-hy(1:ie-1));
exSwx-zxI
ez(ib)=rbc;
E l.eK9L
o|n;{zT"
%***********************************************************************
;;UsHhbhI
% Update magnetic fields
7>7n|N
%***********************************************************************
nUONI+6Z/
n3J,`1*ct
hy(1:ie)=hy(1:ie)+ez(2:ib)-ez(1:ie);
n @@tO#!\
vr47PM2al
%***********************************************************************
P/~dY[6m
% Visualize fields
w0js_P-uv
%***********************************************************************
gHUW1E
HSG9|}$
.-s!} P"
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1
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cem-uestc
rf币
+5
你发了优秀贴子+2~3
2008-06-17
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cem-uestc
UID :9061
注册:
2008-03-07
登录:
2019-01-05
发帖:
2575
等级:
荣誉管理员
1楼
发表于: 2008-06-17 21:41:49
Matlab代码值得学习,制作仿真动画的好参考matlab代码,其价值超过FDTD代码,奖励
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