天线阵代码
.pudn./downloads164/sourcecode/math/detail750575.htm
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一、
clc
clear all
f=3e9;
N1=4;N2=8;N3=12;
a=pi/2; %馈电相位差
i=1; %天线电流值
lambda=(3e8)/f; %lambda=c/f 波长
d=lambda/2;
beta=2.*pi/lambda;
W=-2*pi:0.001:2*pi;
y1=sin((N1.*W./2))./(N1.*(sin(W./2))); %归一化阵因子
y1=abs(y1);
r1=max(y1);
y2=sin((N2.*W./2))./(N2.*(sin(W./2))); %归一化阵因子
y2=abs(y2);
r2=max(y2);
y3=sin((N3.*W./2))./(N3.*(sin(W./2))); %归一化阵因子
y3=abs(y3);
r3=max(y3);
%归一化阵因子绘图程序,
figure(1)
subplot(311);plot(W,y1) ; grid on; %绘出N=4等幅等矩阵列的归一化阵因子
xlabel('f=3GHz,N=4,d=1/2波长,a=π/2')
subplot(312);plot(W,y2) ; grid on; %绘出N=8等幅等矩阵列的归一化阵因子
xlabel('f=3GHz,N=8,d=1/2波长,a=π/2')
subplot(313);plot(W,y3) ; grid on; %绘出N=12等幅等矩阵列的归一化阵因子
xlabel('f=3GHz,N=12,d=1/2波长,a=π/2')
%---------------------
%只有参数N改变的天线方向图
t=0:0.01:2*pi;
W=a+(beta.*d.*cos(t));
z1=(N1/2).*(W);
z2=(1/2).*(W);
W1=sin(z1)./(N1.*sin(z2)); %非归一化的阵因子K1
K1=abs(W1);
%----------------------
W=a+(beta.*d.*cos(t));
z3=(N2/2).*(W);
z4=(1/2).*(W);
W2=sin(z3)./(N2.*sin(z4)); %非归一化的阵因子K2
K2=abs(W2);
%-------------------------
W=a+(beta.*d.*cos(t));
z5=(N3/2).*(W);
z6=(1/2).*(W);
W3=sin(z5)./(N3.*sin(z6)); %非归一化的阵因子K3
K3=abs(W3);
%--------------------绘图函数
figure(2)
subplot(131);polar(t,K1);xlabel('f=3GHz,N=4,d=1/2波长,a=π/2'); subplot(132);polar(t,K2);xlabel('f=3GHz,N=8,d=1/2波长,a=π/2'); subplot(133);polar(t,K3);xlabel('f=3GHz,N=12,d=1/2波长,a=π/2'); %----------------------
%只有阵列单元方向角a改变的天线方向图
N4=10;d1=lambda/4;a1=0;a2=pi/2;a3=pi/2+pi/10;
A=a1+(beta.*d1.*cos(t));
x1=(N4/2).*(A);
x2=(1/2).*(A);
A1=sin(x1)./(N4.*sin(x2)); %非归一化的阵因子K4
K4=abs(A1);
%---------------------------
B=a2+(beta.*d1.*cos(t));
y_1=(N4/2).*(B);
y_2=(1/2).*(B);
B1=sin(y_1)./(N4.*sin(y_2)); %非归一化的阵因子K5
K5=abs(B1);
%----------------------------
C=a3+(beta.*d1.*cos(t));
v1=(N4/2).*(C);
v2=(1/2).*(C);
C1=sin(v1)./(N4.*sin(v2)); %非归一化的阵因子K6
K6=abs(C1);
%--------------------------绘图函数
figure(3)
subplot(131);polar(t,K4);xlabel('f=3GHz,N=10,d=1/4波长,a=0');
subplot(132);polar(t,K5);xlabel('f=3GHz,N=10,d=1/4波长,a=π/2'); subplot(133);polar(t,K6);xlabel('f=3GHz,N=10,d=1/4波长,a=π/2+π/10'); %----------------------------------------------------------------------
%只有阵列单元间隔d改变的天线方向图
N5=20;d2=lambda/4;d3=lambda/2;d4=0.7*lambda;a4=pi/2;
D=a4+(beta.*d2.*cos(t));
p1=(N5/2).*(D);
p2=(1/2).*(D);
D1=sin(p1)./(N5.*sin(p2)); %非归一化的阵因子K7
K7=abs(D1);
%------------------------------
E=a4+(beta.*d3.*cos(t));
q1=(N5/2).*(E);
q2=(1/2).*(E);
E1=sin(q1)./(N5.*sin(q2)); %非归一化的阵因子K8
K8=abs(E1);
%-------------------------------
F=a4+(beta.*d4.*cos(t));
r_1=(N5/2).*(F);
r_2=(1/2).*(F);
F1=sin(r_1)./(N5.*sin(r_2)); %非归一化的阵因子K9
K9=abs(F1);
%-----------------------绘图函数
figure(4)
subplot(131);polar(t,K7);xlabel('f=3GHz,N=20,d=1/4波长,a=π/2'); subplot(132);polar(t,K8);xlabel('f=3GHz,N=20,d=1/2波长,a=π/2'); subplot(133);polar(t,K9);xlabel('f=3GHz,N=20,d=0.7波长,a=π/2');
%--------------------------------------------------------------------------
%---------------------------------------3D-天线方向图
n_tehta = 130; %-------------------- 采样视角点的仰角
n_phi = 130; %--------------------采样点的方向角
[tehta,phi]=meshgrid(eps:pi./(n_tehta-1):pi,... %meshgrid函数为矩形区域的设定围是epf 0:2*pi./(n_phi-1):2*pi) ; t3=tehta; %-------------只有参数N改变的天线方向3D图 M=a+(beta.*d.*cos(t3)); %----N1=4;N2=8;N3=12; z_1=(N1/2).*(M); z_2=(1/2).*(M); M1=sin(z_1)./(N1.*sin(z_2)); %非归一化的阵因子K1 K_1=abs(M1); radio_1 =K_1; X1=radio_1.*sin(tehta).*cos(phi); Y1=radio_1.*sin(tehta).*sin(phi); Z1=radio_1.*cos(tehta); %----------------------------------- M=a+(beta.*d.*cos(t3)); z_3=(N2/2).*(M); z_4=(1/2).*(M); M2=sin(z_3)./(N2.*sin(z_4)); %非归一化的阵因子K2 K_2=abs(M2); radio_2 =K_2; X2=radio_2.*sin(tehta).*cos(phi); Y2=radio_2.*sin(tehta).*sin(phi); Z2=radio_2.*cos(tehta); %------------------------------------- M=a+(beta.*d.*cos(t3)); z_5=(N3/2).*(M); z_6=(1/2).*(M); M3=sin(z_5)./(N3.*sin(z_6)); %非归一化的阵因子K3 K_3=abs(M3); radio_3 =K_3; X3=radio_3.*sin(tehta).*cos(phi); Y3=radio_3.*sin(tehta).*sin(phi); Z3=radio_3.*cos(tehta); %------------------------------------3D绘图函数 figure(5) surf(X1,Y1,Z1); %三维绘图函数surf,采用伪彩色表示曲面的高度camlight right light colorbar axis image rotate3D on title('f=3GHz,N=4,d=1/2波长,a=π/2'); figure(6) surf(X2,Y2,Z2); camlight right light colorbar axis image rotate3D on title('f=3GHz,N=8,d=1/2波长,a=π/2'); figure(7) surf(X3,Y3,Z3) camlight right light colorbar axis image rotate3D on title('f=3GHz,N=12,d=1/2波长,a=π/2'); %---------------------------------------------- %--------------------只有阵列单元方向角a改变的天线方向图N4=10;d1=lambda/4;a1=0;a2=pi/2;a3=pi/2+pi/10; A_3d=a1+(beta.*d1.*cos(t3)); x_1=(N4/2).*(A_3d); x_2=(1/2).*(A_3d); A_1=sin(x_1)./(N4.*sin(x_2)); %非归一化的阵因子K4 K_4=abs(A_1); radio_4 =K_4; X4=radio_4.*sin(tehta).*cos(phi); Y4=radio_4.*sin(tehta).*sin(phi); Z4=radio_4.*cos(tehta); %----------------------------------- B_3d=a2+(beta.*d1.*cos(t3)); y_1_3d=(N4/2).*(B_3d); y_2_3d=(1/2).*(B_3d); B_1=sin(y_1_3d)./(N4.*sin(y_2_3d)); %非归一化的阵因子K5 K_5=abs(B_1); radio_5 =K_5; X5=radio_5.*sin(tehta).*cos(phi); Y5=radio_5.*sin(tehta).*sin(phi); Z5=radio_5.*cos(tehta); %------------------------------------ C_3d=a3+(beta.*d1.*cos(t3)); v_1=(N4/2).*(C_3d); v_2=(1/2).*(C_3d); C_1=sin(v_1)./(N4.*sin(v_2)); %非归一化的阵因子K6 K_6=abs(C_1); radio_6 =K_6; X6=radio_6.*sin(tehta).*cos(phi); Y6=radio_6.*sin(tehta).*sin(phi); Z6=radio_6.*cos(tehta); %----------------------------------- figure(8) surf(X4,Y4,Z4); %三维绘图函数surf,采用伪彩色表示曲面的高度camlight right light colorbar axis image rotate3D on title('f=3GHz,N=10,d=1/4波长,a=0'); figure(9) surf(X5,Y5,Z5); camlight right light colorbar axis image rotate3D on title('f=3GHz,N=10,d=1/4波长,a=π/2'); figure(10) surf(X6,Y6,Z6) camlight right light colorbar axis image rotate3D on title('f=3GHz,N=10,d=1/4波长,a=π/2+π/10'); %--------------------------------------------- %-------------------只有阵列单元间隔d改变的天线方向3D图 N5=20;d2=lambda/4;d3=lambda/2;d4=0.7*lambda;a4=pi/2; D_3d=a4+(beta.*d2.*cos(t3)); p_1=(N5/2).*(D_3d); p_2=(1/2).*(D_3d); D_1=sin(p_1)./(N5.*sin(p_2)); %非归一化的阵因子K7 K_7=abs(D_1); radio_7 =K_7; X7=radio_7.*sin(tehta).*cos(phi); Y7=radio_7.*sin(tehta).*sin(phi); Z7=radio_7.*cos(tehta); %--------------------------------------- E_3d=a4+(beta.*d3.*cos(t3)); q_1=(N5/2).*(E_3d); q_2=(1/2).*(E_3d); E_1=sin(q_1)./(N5.*sin(q_2)); %非归一化的阵因子K8 K_8=abs(E_1); radio_8 =K_8; X8=radio_8.*sin(tehta).*cos(phi); Y8=radio_8.*sin(tehta).*sin(phi); Z8=radio_8.*cos(tehta); %------------------------------------------ F_3d=a4+(beta.*d4.*cos(t3)); r_1_3d=(N5/2).*(F_3d); r_2_3d=(1/2).*(F_3d); F_1=sin(r_1_3d)./(N5.*sin(r_2_3d)); %非归一化的阵因子K9 K_9=abs(F_1); radio_9 =K_9; X9=radio_9.*sin(tehta).*cos(phi); Y9=radio_9.*sin(tehta).*sin(phi); Z9=radio_9.*cos(tehta); %----------------------------------- figure(11) surf(X7,Y7,Z7); %三维绘图函数surf,采用伪彩色表示曲面的高度camlight right light colorbar axis image rotate3D on title('f=3GHz,N=20,d=1/4波长,a=π/2'); figure(12) surf(X8,Y8,Z8); camlight right light colorbar axis image rotate3D on title('f=3GHz,N=20,d=1/2波长,a=π/2'); figure(13) surf(X9,Y9,Z9) camlight right light colorbar axis image rotate3D on title('f=3GHz,N=20,d=0.7波长,a=π/2'); 二、 %-----------------均匀直线阵列天线的应用之一:边射阵 clc clear all f=3e10; %30GHz,厘米波 i=1; %天线电流值 lambda=(3e8)/f; %lambda=c/f 波长 beta=2.*pi/lambda; N=15; t=0:0.01:2*pi; d1=lambda/4; %没有栅瓣效应的边射阵,即间隔d<波长 W1=beta.*d1.*cos(t); %定义kdcos(方向角) z1=(N/2).*W1; z2=(1/2).*W1; F1=sin(z1)./(N.*sin(z2)); K1=abs(F1); d2=lambda*1.5; %有栅瓣现象的边射阵,即间隔d>波长 W2=beta.*d2.*cos(t); %定义kdcos(方向角) z3=(N/2).*W2; z4=(1/2).*W2; F2=sin(z3)./(N.*sin(z4)); K2=abs(F2); figure(1) subplot(121);polar(t,K1);title('边射阵f=30GHz,N=15,d=1/4波长'); subplot(122);polar(t,K2);title('边射阵(有栅瓣)f=30GHz,N=15,d=1.5倍波长'); 三、 %-----------------均匀直线阵列天线的应用之二:普通端射阵 clc clear all f=3e10; %30GHz,厘米波 i=1; %天线电流值 lambda=(3e8)/f; %lambda=c/f 波长 beta=2.*pi/lambda; N=15; t=0:0.01:2*pi; d1=lambda/4; %没有栅瓣效应的普通端射阵,即间隔d<1/2波长 W1=beta.*d1.*cos(t); %定义kdcos(方向角) z1=((N/2).*W1)+N/2*beta*d1; z2=((1/2).*W1)+1/2*beta*d1; F1=sin(z1)./(N.*sin(z2)); K1=abs(F1); d2=lambda*0.7; %有栅瓣现象的普通端射阵,即间隔d>1/2波长 W2=beta.*d2.*cos(t); %定义kdcos(方向角) z3=((N/2).*W2)+N/2*beta*d2; z4=((1/2).*W2)+1/2*beta*d2; F2=sin(z3)./(N.*sin(z4)); K2=abs(F2); figure(2) subplot(121);polar(t,K1);title('普通端射阵f=30GHz,N=15,d=1/4波长'); subplot(122);polar(t,K2);title('普通端射阵(有栅瓣)f=30GHz,N=15,d=0.7倍波长'); 四 %-----------------均匀直线阵列天线的应用之三:强方向性端射阵 clc clear all f=3e10; %30GHz,厘米波 i=1; %天线电流值 lambda=(3e8)/f; %lambda=c/f 波长 beta=2.*pi/lambda; N=15; t=0:0.01:2*pi; d1=lambda/4; %没有栅瓣效应的强方向性端射阵,即间隔d<(1/2波 长)*(1-1/N) W1=beta.*d1.*cos(t); %定义kdcos(方向角) z1=((N/2).*W1)+N/2*(beta*d1+pi/N); z2=((1/2).*W1)+1/2*(beta*d1+pi/N); F1=sin(pi/2/N).*sin(z1)./(sin(z2)); K1=abs(F1); d2=lambda*0.5; %有栅瓣现象的强方向性端射阵,即间隔d>1/2波长*(1-1/N) W2=beta.*d2.*cos(t); %定义kdcos(方向角) z3=((N/2).*W2)+N/2*(beta*d2+pi/N); z4=((1/2).*W2)+1/2*(beta*d2+pi/N); F2=sin(pi/2/N).*sin(z3)./(sin(z4)); K2=abs(F2); figure(3) subplot(121);polar(t,K1);title('强方向性端射阵f=30GHz,N=15,d=1/4波长'); subplot(122);polar(t,K2);title('强方向性端射阵(有栅瓣) f=30GHz,N=15,d=0.5倍波长');