The landing control of the unmanned aerial vehicles is a very difficult task having in mind both the external disturbances and their strong nonlinear dynamics with channel interferences. Motivated by this fact, this paper deals with the design of a novel automatic landing system (ALS) for a tailless and fixed blended wing unmanned aerial vehicle (UAV) having mobile centre of mass. By using the backstepping and the dynamic inversion control techniques, a novel auto-landing system is designed and software validated to control the aircraft during all the three landing phases (final approach, glide slope phase, flare) and handle the external disturbances such as the atmospheric turbulences and the errors of the measurement sensors. The dynamics of the aircraft involves the interconnection between the motions in the longitudinal and lateral-directional planes in contrast to other works where the dynamics has been separately linearized before developing of the control laws. The auto-landing system consists of two controllers (for the attitude angles and the forward speed of the UAV), an adaptive observer (for the estimation of the atmospheric turbulences), four reference models (to obtain the desired attitude angles and forward speed). This novel control architecture also uses the desired landing geometry and the operating conditions associated to a default trajectory defined by means of the calculated attitude angles and velocity of the UAV. The first controller (based on the backstepping control technique) provides the deflections of the three control surfaces, while the second one (based on the dynamic inversion technique) provides the throttle command to maintain a constant airspeed. The deviation of the UAV from the runway is cancelled and the desired landing trajectory is followed accurately. The results of the numerical simulations show the fulfilment of all the control objectives, including here the steady and the transient performances of the tracking errors, as well as the robustness relative to the atmospheric turbulences, the errors of the measurement sensors, and the motion of the mass centre.
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