“…Let us consider two main reference frames: an inertial coordinate frame O e x e y e z e fixed to ground and a body fixed coordinate frame O b x b y b z b . The 6‐DOF airframe dynamics of a quadrotor involves translational and rotational motions, described by where P i =[ x i , y i , z i ] T and V i =[ u i , v i , w i ] T represent the position and velocity of the i th quadrotor in the inertial frame, and Θ i =[ ϕ i , θ i , ψ i ] T and Ω i =[ p i , q i , r i ] T represent the Euler angles and angular rates of the i th quadrotor in the body frame. g is the acceleration due to the gravity, and d Vi =[ d ui , d vi , d wi ] T as well as d Ω i =[ d pi , d qi , d ri ] T are composite disturbance.…”