syms th psi phi real
% Set up the direction cosine matrix for phi theta and psi ...
C1 = [ 1 0 0 ; 0 cos(phi) sin(phi) ; 0 -sin(phi) cos(phi) ];
C2 = [ cos(th) 0 -sin(th); 0 1 0 ; sin(th) 0 cos(th) ];
C3 = [ cos(psi) sin(psi) 0; -sin(psi) cos(psi) 0; 0 0 1 ];
CBI = C1*C2*C3
% Show that dCBI(:)/dt = dCBI/dphi*p + dCBI/dth*q + dCBI/psi*r
% = -Omega*CBI
% = [Cx1*omega Cx2*omega Cx3*omega]
syms p q r real
omega = [p q r]';
Omega = [0 r -q; -r 0 p; q -p 0];
% Set up the cross product matrices for the DCM x omega ...
Cx1=[0 -CBI(3,1) CBI(2,1);CBI(3,1) 0 -CBI(1,1); -CBI(2,1) CBI(1,1) 0]
Cx2=[0 -CBI(3,2) CBI(2,2);CBI(3,2) 0 -CBI(1,2); -CBI(2,2) CBI(1,2) 0]
Cx3=[0 -CBI(3,3) CBI(2,3);CBI(3,3) 0 -CBI(1,3); -CBI(2,3) CBI(1,3) 0]
C = [Cx1;Cx2;Cx3]
Cdot1 = Omega*CBI
pause
Cdot2 = [C(1:3,:)*omega C(4:6,:)*omega C(7:9,:)*omega]
pause
simplify(Cdot1-Cdot2)
pause
% Show that C'C=2I ...
simplify(C'*C)
pause
% Show that C'CBI(:) = 0 ...
simplify(C'*CBI(:))
pause