xitongfangcheng.asv

LQR源程序

H=axes('Position', [0, 0, 1, 1], 'Visible', 'off');

str{1}='\fontname{隶书}动力学方程';									%<11>
str{2}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (1)';
str{3}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (2)';
str{4}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (3)';
str{5}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (4)';
str{6}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (5)';
str{7}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (6)';	
str{8}='\fontname{隶书}运动学方程';
str{9}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (7)';
str{10}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (8)';
str{11}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (9)';
str{12}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (10)';
str{13}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (11)';
str{14}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (12)';
str{15}='\fontname{隶书}弹道方程';
str{16}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (13)';
str{17}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (14)';
str{18}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (15)';
str{19}='\fontname{隶书}动力角方程';
str{20}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (16)';
str{21}='mu+qr = 1 - \beta^{-1}e^{-\zetat}sin(\betat + \theta) (17)';
str{22}='其中：\Psi,\Theta,\Phi 是姿态角 ;';

%<15>
%
set(gcf, 'CurrentAxes',H)													%<18>
text(0.04, 0.52, str, 'FontSize', 14)									%<19>