“…Let I be the inertial reference frame, B be the local reference frame, ⃗ d = X Y Z T be the vector of coordinates X, Y, Z ∈ R in I; ⃗ ρ = Φ Θ Ψ T be the vector of Euler angles Φ, Θ, Ψ ∈ R with respect to the North-East-Down frame (NED); ⃗ Ω = p q r T be the vector of the body roll, pitch and yaw rotational rates; and ⃗ τ = L M N T be the vector of moments L, M, N ∈ R around the roll, pitch and yaw axes. The attitude dynamics is presented in (1) [22], [23], where S (⃗ ρ) is defined as T(η) by Falconí et al [22]. The dynamics of the rotational rates are defined by Euler's equation [22], [23] in (2), where J ∈ R 3×3 is the inertia matrix of the quadrotor.…”