📄 test_align_compass.m
字号:
clear
close
glvs;
ws2 = glv.g0/glv.Re; % 修拉周期平方
xi = sqrt(2)/2; Td = 20; % 水平调平参数k1,k2,k3
sigma = 2*pi*xi/(Td*sqrt(1-xi^2));
k1 = 3*sigma; k2 = sigma^2*(2+1/xi^2)/ws2-1; k3 = sigma^3/(glv.g0*xi^2);
xi = sqrt(2)/2; Td = 50; % 罗经回路控制参数kz1,kz2,kz3
sigma = 2*pi*xi/(Td*sqrt(1-xi^2));
kz1 = 2*sigma; kz4 = kz1; kz2 = 4*sigma^2/ws2-1; kz3 = 4*sigma^4/glv.g0;
VE = 0; VN = 0; PE = 0; PN = 0; wnc = zeros(3,1); % 状态初始值
L = 34*glv.deg; pos = [L; 0; 0]; % 初始位置
[wnie, wnen, RMh, RNh, gn] = earth(pos, [0;0;0]);
eb = [.01; .01; -.01]*glv.dph; web = [0.001; 0.001; 0.001]*glv.dph; % 陀螺漂移
db = [100; -100; 100]*glv.ug; wdb = [10; 10; 10]*glv.ug; % 加速度计零偏
att = [0; 0; 30]*glv.deg; qnb0 = a2qnb(att); % 姿态真值
phi = [-10.00; 10.00; 60.0]*glv.min;
qnb = qaddphi(qnb0, phi); % 加入姿态误差的计算四元数初值
Ts = .1; % 仿真步长
t = 300; % 总时间长度
len = fix(t/Ts); phik=zeros(len,3);
for k=1:len
wbib = qmulv(qconj(qnb0),wnie)+eb+web.*randn(3,1); % 陀螺采样角速度(假设载体静止)
fbsf = qmulv(qconj(qnb0),-gn)+db+wdb.*randn(3,1); % 加速度计采样比力
qnb = qmul( qnb, rv2q((wbib-qmulv(qconj(qnb),wnie+wnc))*Ts) ); % 带反馈控制项wnc的姿态更新
fn = qmulv(qnb, fbsf); % 比力变换
phik(k,:) = qq2phi(qnb, qnb0)';
if k<(50/Ts) % 前50s水平调平
VE = VE + (fn(1)-k1*VE)*Ts;
PE = PE + VE*k3*Ts;
wnc(2,1) = VE*(1+k2)/glv.Re + PE;
VN = VN + (fn(2)-k1*VN)*Ts;
PN = PN + VN*k3*Ts;
wnc(1,1) = -VN*(1+k2)/glv.Re - PN;
else % 罗经对准
VE = VE + (fn(1)-k1*VE)*Ts;
PE = PE + VE*k3*Ts;
wnc(2,1) = VE*(1+k2)/glv.Re + PE;
VN = VN + (fn(2)-k1*VN)*Ts;
PN = PN + VN*k3*Ts;
VN = VN + (fn(2)-kz1*VN)*Ts;
wnc(1,1) = -VN*(1+kz2)/glv.Re;
wnc(3,1) = (VN*kz3*Ts/wnie(2)+wnc(3,1))/(1+kz4*Ts);
end
end
time = [1:length(phik)]*Ts;
figure
subplot(3,1,1), plot(time,phik(:,1)/glv.min), ylabel('\it\phi_E\rm / arcmin'); grid on
subplot(3,1,2), plot(time,phik(:,2)/glv.min), ylabel('\it\phi_N\rm / arcmin'); grid on
subplot(3,1,3), plot(time,phik(:,3)/glv.min), ylabel('\it\phi_U\rm / arcmin'); grid on
xlabel('\itt \rm / s');
⌨️ 快捷键说明
复制代码
Ctrl + C
搜索代码
Ctrl + F
全屏模式
F11
切换主题
Ctrl + Shift + D
显示快捷键
?
增大字号
Ctrl + =
减小字号
Ctrl + -