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下载了一个fdtd算法的源程序,结果里面代码 ..
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FDTD
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下载了一个fdtd算法的源程序,结果里面代码中有*****is([-1.0 1.0]);这样的语句看不懂
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zhuoruizhuc
UID :94892
注册:
2012-05-30
登录:
2012-06-03
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6
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发表于: 2012-05-31 06:57:06
%***********************************************************************
`mHOgS>|
% 3-D FDTD code with PEC boundaries
W> -E.#!_
%***********************************************************************
dp%pbn6w
%
1Ag ;s
% Program author: Susan C. Hagness
8bKWIN g_n
% Department of Electrical and Computer Engineering
r>:7${pF
% University of Wisconsin-Madison
cM7k) {
% 1415 Engineering Drive
1RUbY>K#U
% Madison, WI 53706-1691
(w@MlMk
% 608-265-5739
6pdl,5[x-
%
hagness@engr.wisc.edu
,oi`BOh
%
c#4L*$ViF
% Date of this version: February 2000
?H86Wbz
%
1\.zOq#
% This MATLAB M-file implements the finite-difference time-domain
o-e,
% solution of Maxwell's curl equations over a three-dimensional
"8iyMP%8
% Cartesian space lattice comprised of uniform cubic grid cells.
~IJZM`gN
%
ba)YbP[
% To illustrate the algorithm, an air-filled rectangular cavity
)DZ-vnZ#t0
% resonator is modeled. The length, width, and height of the
> Qbc(}w
% cavity are 10.0 cm (x-direction), 4.8 cm (y-direction), and
=='{[[J
% 2.0 cm (z-direction), respectively.
yPxG`w'
%
i[BR(D&l_p
% The computational domain is truncated using PEC boundary
+68K[s,FD
% conditions:
t5B|c<Hb\
% ex(i,j,k)=0 on the j=1, j=jb, k=1, and k=kb planes
l!2Z`D_MD
% ey(i,j,k)=0 on the i=1, i=ib, k=1, and k=kb planes
94k)a8-!
% ez(i,j,k)=0 on the i=1, i=ib, j=1, and j=jb planes
d ;7pri)B
% These PEC boundaries form the outer lossless walls of the cavity.
S&)) 0d
%
ek.WuOs
% The cavity is excited by an additive current source oriented
re 1k]
% along the z-direction. The source waveform is a differentiated
Z!=Pc$?
% Gaussian pulse given by
W$VCST
% J(t)=-J0*(t-t0)*exp(-(t-t0)^2/tau^2),
gp&& c,
% where tau=50 ps. The FWHM spectral bandwidth of this zero-dc-
.0*CT:1=0
% content pulse is approximately 7 GHz. The grid resolution
cTIwA:)D
% (dx = 2 mm) was chosen to provide at least 10 samples per
8UY=}R2C
% wavelength up through 15 GHz.
}+RF~~H/
%
UEYM;$_@4o
% To execute this M-file, type "fdtd3D" at the MATLAB prompt.
zt>_)&b
% This M-file displays the FDTD-computed Ez fields at every other
H6 f; BS
% time step, and records those frames in a movie matrix, M, which
'Tan6Qa
% is played at the end of the simulation using the "movie" command.
_I}L$
%
{@F["YPxy
%***********************************************************************
r/$)c_x`
R_*D7|v
clear
:R*^Izs=
%***********************************************************************
O[(HE8E
% Fundamental constants
?e|:6a+[f
%***********************************************************************
f/WM}Hpj
/KvPiQ%
cc=2.99792458e8; %speed of light in free space
R&|)y:bg|
muz=4.0*pi*1.0e-7; %permeability of free space
o_Kc nVQ\
epsz=1.0/(cc*cc*muz); %permittivity of free space
s2v#evI`+
gW pT:tX-
%***********************************************************************
Kac j
% Grid parameters
08n%% F
%***********************************************************************
j{w,<Wt>
ie=50; %number of grid cells in x-direction
Y1ilH-8
je=24; %number of grid cells in y-direction
+(P43XO08
ke=10; %number of grid cells in z-direction
wj:3
ib=ie+1;
C.e|VzQa
jb=je+1;
Jc#)T;#6
kb=ke+1;
byj mH
E `j5y(44
is=26; %location of z-directed current source
F@(}=w^(A
js=13; %location of z-directed current source
f;XsShxr
huD\dmQ:]
kobs=5;
a:%5.!Vd
dx=0.002; %space increment of cubic lattice
'UG}E@G
dt=dx/(2.0*cc); %time step
0}7Rm>
n; '~"AG)
nmax=500; %total number of time steps
<GmrKdM
_(kwD^x6O{
%***********************************************************************
l:Xf(TLa
% Differentiated Gaussian pulse excitation
=O:ek#Bp
%***********************************************************************
uV$d7(N}"
> FcA,
rtau=50.0e-12;
IEr`6|X
tau=rtau/dt;
x^#{2}4u
ndelay=3*tau;
y<x_v )k-
srcconst=-dt*3.0e+11;
BNoCE!
64?$TT
%***********************************************************************
3!w>"h0(
% Material parameters
=|&"/$+s
%***********************************************************************
|iJZC
9n\#s~,
eps=1.0;
LOG*K;v3
sig=0.0;
B+[Q$Q"
T2PFE4+Dp
%***********************************************************************
V5@[7ncVf
% Updating coefficients
E9*?G4P{l
%***********************************************************************
M |kDys
-:p1gg&
ca=(1.0-(dt*sig)/(2.0*epsz*eps))/(1.0+(dt*sig)/(2.0*epsz*eps));
Olh%"=*;
cb=(dt/epsz/eps/dx)/(1.0+(dt*sig)/(2.0*epsz*eps));
86 /i~s
da=1.0;
-V_S4|>
db=dt/muz/dx;
U)=Z&($T
%***********************************************************************
#2'&=?J1r
% Field arrays
Py0i%pZ
%***********************************************************************
)n[Mh!mn
ex=zeros(ie,jb,kb);
E6-(q!"A
ey=zeros(ib,je,kb);
N$a-i
ez=zeros(ib,jb,ke);
>Pd23TsN
hx=zeros(ib,je,ke);
@.@#WHde
hy=zeros(ie,jb,ke);
ITqigGan%
hz=zeros(ie,je,kb);
*rKv`nva5
%***********************************************************************
n~i4yn=
% Movie initialization
3rdxXmx
%***********************************************************************
5@rqU(]<
tview(:,:)=ez(:,:,kobs);
\R6T"U
sview(:,:)=ez(:,js,:);
|nZB/YZt
"/-v 9
subplot('position',[0.15 0.45 0.7 0.45]),pcolor(tview');
Q/`o6xv
shading flat;
C^:&3,
*****is([-1.0 1.0]);
Wq&c,H
colorbar;
m]}"FMH$
axis image;
Uk ;.Hrt.
title(['Ez(i,j,k=5), time step = 0']);
[a*>@IR
xlabel('i coordinate');
Kf<_A{s
ylabel('j coordinate');
#_sVB~sn@
subplot('position',[0.15 0.10 0.7 0.25]),pcolor(sview');
1% %Tm"
shading flat;
<).qe Z
*****is([-1.0 1.0]);
4xn^`xf9
colorbar;
`a-T95IFy
axis image;
aNU%OeQA
title(['Ez(i,j=13,k), time step = 0']);
>b](v)
xlabel('i coordinate');
_7HJ'
ylabel('k coordinate');
{QkH%jj
rect=get(gcf,'Position');
)g^Ewzy^X
rect(1:2)=[0 0];
s/0FSv x
M=moviein(nmax/2,gcf,rect);
Zo ReyY2
(lsod#wEMg
%***********************************************************************
\iSBLU
% BEGIN TIME-STEPPING LOOP
D)cwttH
%***********************************************************************
ouZ9oy(}a
for n=1:nmax
%9)J-B
%***********************************************************************
{#Cm> @')
% Update electric fields
KCT"a:\
%***********************************************************************
OWfj<#}t+
"$;:dfrU
ex(1:ie,2:je,2:ke)=ca*ex(1:ie,2:je,2:ke)+...
|i}g7
cb*(hz(1:ie,2:je,2:ke)-hz(1:ie,1:je-1,2:ke)+...
B&j+fi
hy(1:ie,2:je,1:ke-1)-hy(1:ie,2:je,2:ke));
/ hdl
ey(2:ie,1:je,2:ke)=ca*ey(2:ie,1:je,2:ke)+...
b:I5poI3
cb*(hx(2:ie,1:je,2:ke)-hx(2:ie,1:je,1:ke-1)+...
vrx3O
hz(1:ie-1,1:je,2:ke)-hz(2:ie,1:je,2:ke));
0DT2qM[,
ez(2:ie,2:je,1:ke)=ca*ez(2:ie,2:je,1:ke)+...
?S:_J!vX{
cb*(hx(2:ie,1:je-1,1:ke)-hx(2:ie,2:je,1:ke)+...
Q</HFpE
hy(2:ie,2:je,1:ke)-hy(1:ie-1,2:je,1:ke));
*0ntx$M-w
JY8pV+q @=
ez(is,js,1:ke)=ez(is,js,1:ke)+...
HD|)D5wH|
srcconst*(n-ndelay)*exp(-((n-ndelay)^2/tau^2));
dg8\(G
%***********************************************************************
BQf+1Ly&
% Update magnetic fields
1/J*ki+?
%***********************************************************************
6x8|v7cMH
hx(2:ie,1:je,1:ke)=hx(2:ie,1:je,1:ke)+...
b#j5fEY
db*(ey(2:ie,1:je,2:kb)-ey(2:ie,1:je,1:ke)+...
,.F+x}
ez(2:ie,1:je,1:ke)-ez(2:ie,2:jb,1:ke));
"g[UX{L
hy(1:ie,2:je,1:ke)=hy(1:ie,2:je,1:ke)+...
YWF<2l.
db*(ex(1:ie,2:je,1:ke)-ex(1:ie,2:je,2:kb)+...
:?W:'% (`[
ez(2:ib,2:je,1:ke)-ez(1:ie,2:je,1:ke));
;H|M)z#[Z
hz(1:ie,1:je,2:ke)=hz(1:ie,1:je,2:ke)+...
- & r{%7
db*(ex(1:ie,2:jb,2:ke)-ex(1:ie,1:je,2:ke)+...
K%Ml2V
ey(1:ie,1:je,2:ke)-ey(2:ib,1:je,2:ke));
eA^|B zU
%************************************ ..
}CqIKoX.
D$ z!wV
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zhuoruizhuc
UID :94892
注册:
2012-05-30
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2012-06-03
发帖:
6
等级:
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1楼
发表于: 2012-05-31 06:57:49
谁能帮我改一下啊,万分感谢
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whynot910
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17499
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2楼
发表于: 2019-03-11 20:27:19
这是什么语言的代码呢
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