IIR滤波器matlab源程序

IIR的matlab源程序

IIR滤波器matlab源程序

（1）IIR一阶低通滤波器

clear;

fi=1;fs=10;Gc2=0.9;

wc=2*pi*fi/fs;

omegac=tan(wc/2);

alpha=(sqrt(Gc2)/sqrt(1-Gc2))*omegac;

a=(1-alpha)/(1+alpha);

b=(1-a)/2;

w=0:pi/300:pi;

Hw2=alpha^2./(alpha^2+(tan(w/2)).^2);

plot(w/pi,Hw2);

grid;

hold on;

（2）一阶高通滤波器

clear;

fi=1;fs=10;Gc2=0.5;

wc=2*pi*fi/fs;

omegac=tan(wc/2);

alpha=(sqrt(1-Gc2)/(sqrt(Gc2)))*omegac;

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IIR的matlab源程序

a=(1-alpha)/(1+alpha);

b=(1+a)/2;

w=0:pi/300:pi;

Hw2=(tan(w/2).^2)./(alpha^2+(tan(w/2)).^2);

plot(w/pi,Hw2);

grid;

hold on;

（3）Notch 嵌波滤波器

clear;

Gb2=0.5;

w0=0.35*pi;

deltaw=0.1*pi;

b=1/(1+tan(deltaw/2)*(sqrt(1-Gb2)/sqrt(Gb2)));

B=[1 -2*cos(w0) 1].*b;

A=[1 -2*b*cos(w0) (2*b-1)];

w=0:pi/500:pi;

H=freqz(B,A,w);

plot(w/pi,abs(H));

grid;

（4）Peak 滤波器

clear;

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IIR的matlab源程序

Ac=3;

Gb2=10^(-Ac/10);

w0=0.35*pi;

deltaw=0.1*pi;

b=1/(1+tan(deltaw/2)*(sqrt(Gb2)/sqrt(1-Gb2)));

B=[1 0 -1].*(1-b);

A=[1 -2*b*cos(w0) (2*b-1)];

w=0:pi/500:pi;

H=freqz(B,A,w);

plot(w/pi,abs(H));

grid;

（5）IIR低通滤波（Butterworth）

% IIR Lowpass Use Butterworth

clear;

fs=20;fpass=4;fstop=5;

Ap=0.5;As=10;

wp=2*pi*fpass/fs;ws=2*pi*fstop/fs;

omegap=tan(wp/2);omegas=tan(ws/2);

ep=sqrt(10^(Ap/10)-1);

es=sqrt(10^(As/10)-1);

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IIR的matlab源程序

N=ceil(log(es/ep)/log(omegas/omegap));

omega0=omegap/ep^(1/N);

K=floor(N/2);

for i=1:K

theta(i)=pi*(N-1+2*i)/(2*N);

end

for i=1:K

G(i)=omega0^2/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a1(i)=2*(omega0^2-1)/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a2(i)=(1+2*omega0*cos(theta(i))+omega0^2)/(1-2*omega0*cos(theta(i))+omega0^2); end

if K<(N/2)

G0=omega0/(omega0+1);a0=(omega0-1)/(omega0+1);

end

w=0:pi/300:pi;

Hw2=1./(1+(tan(w/2)/omega0).^(2*N));

plot(w/pi,Hw2);

grid;

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IIR的matlab源程序

（6）IIR高通滤波（Butterworth）

% IIR Hightpass Use Butterworth

clear;

fs=20;fpass=5;fstop=4;

Ap=0.5;As=10;

wp=2*pi*fpass/fs;ws=2*pi*fstop/fs;

omegap=cot(wp/2);omegas=cot(ws/2);

ep=sqrt(10^(Ap/10)-1);

es=sqrt(10^(As/10)-1);

N=ceil(log(es/ep)/log(omegas/omegap));

omega0=omegap/ep^(1/N);

K=floor(N/2);

for i=1:K

theta(i)=pi*(N-1+2*i)/(2*N);

end

for i=1:K

G(i)=omega0^2/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a1(i)=-2*(omega0^2-1)/(1-2*omega0*cos(theta(i))+omega0^2);

end

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IIR的matlab源程序

for i=1:K

a2(i)=(1+2*omega0*cos(theta(i))+omega0^2)/(1-2*omega0*cos(theta(i))+omega0^2); end

if K<(N/2)

G0=omega0/(omega0+1);a0=-(omega0-1)/(omega0+1);

end

w=(0+eps):pi/300:pi;

Hw2=1./(1+(cot(w/2)/omega0).^(2*N));

plot(w/pi,Hw2);

grid;

（7）IIR带通滤波（Butterworth）

% IIR Bandpass Use Butterworth

clear;

fs=20;fpa=2;fpb=4;fsa=1.5;fsb=4.5;

Ap=0.0877;As=16.9897;

wpa=2*pi*fpa/fs;wpb=2*pi*fpb/fs;wsa=2*pi*fsa/fs;wsb=2*pi*fsb/fs;

c=sin(wpa+wpb)/(sin(wpa)+sin(wpb));

omegap=abs((c-cos(wpb))/sin(wpb));

omegasa=(c-cos(wsa))/sin(wsa);omegasb=(c-cos(wsb))/sin(wsb);

omegas=min(abs(omegasa),abs(omegasb));

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IIR的matlab源程序

ep=sqrt(10^(Ap/10)-1);es=sqrt(10^(As/10)-1);

N=ceil(log(es/ep)/log(omegas/omegap));

omega0=omegap/ep^(1/N);

K=floor(N/2);

for i=1:K

theta(i)=pi*(N-1+2*i)/(2*N);

end

for i=1:K

G(i)=omega0^2/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a1(i)=4*c*(omega0*cos(theta(i))-1)/(1-2*omega0*cos(theta(i))+omega0^2); end

for i=1:K

a2(i)=2*(2*c^2+1-omega0^2)/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a3(i)=-(4*c*(omega0*cos(theta(i))+1))/(1-2*omega0*cos(theta(i))+omega0^2); end

for i=1:K

a4(i)=(1+2*omega0*cos(theta(i))+omega0^2)/(1-2*omega0*cos(theta(i))+omega0^2); end

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IIR的matlab源程序

G0=omega0/(1+omega0);a0(1)=-2*c/(1+omega0);a0(2)=(1-omega0)/(1+omega0); end

w=(0+eps):pi/300:pi;

Hw2=1./(1+((c-cos(w))./(omega0*sin(w))).^(2*N));

plot(w/pi,Hw2);

grid;

（8）IIR带阻滤波（Butterworth）

% IIR Bandstop Use Butterworth

clear;

fs=20;fpa=1.5;fpb=4.5;fsa=2;fsb=4;

Ap=0.5;As=10;

wpa=2*pi*fpa/fs;wpb=2*pi*fpb/fs;wsa=2*pi*fsa/fs;wsb=2*pi*fsb/fs;

c=sin(wpa+wpb)/(sin(wpa)+sin(wpb));

omegap=abs(sin(wpb)/(c-cos(wpb)));

omegasa=sin(wsa)/(cos(wsa)-c);omegasb=sin(wsb)/(cos(wsb)-c);

omegas=min(abs(omegasa),abs(omegasb));

ep=sqrt(10^(Ap/10)-1);es=sqrt(10^(As/10)-1);

N=ceil(log(es/ep)/log(omegas/omegap));

omega0=omegap/ep^(1/N);

K=floor(N/2);

theta=zeros(1,K);

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IIR的matlab源程序

theta(i)=pi*(N-1+2*i)/(2*N);

end

G=zeros(1,K);a1=zeros(1,K);a2=zeros(1,K);

for i=1:K

G(i)=omega0^2/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a1(i)=2*(omega0^2-1)/(1-2*omega0*cos(theta(i))+omega0^2);

end

for i=1:K

a2(i)=(1+2*omega0*cos(theta(i))+omega0^2)/(1-2*omega0*cos(theta(i))+omega0^2); end

if K<(N/2)

G0=omega0/(omega0+1);a0=(omega0-1)/(omega0+1);

end

w=(0+eps):pi/300:pi;

Hw2=1./(1+(sin(w)./(omega0*(c-cos(w)))).^(2*N));

plot(w/pi,Hw2);

grid;

（9）IIR低通滤波（chebyshev 1）

% IIR Lowpass Use Chebyshev Type 1

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