The most probable physical models of hydrogen sensors based on thin stannic oxide films, MOS-structures, and tunnel MOS-diodes are discussed. The emphasis is on the mechanisms of formation of sensor response to hydrogen. The analytical equations describing the dependence of the response on the hydrogen concentration n Н 2 are derived for all types of sensors. The relations describing the dependences of the SnO 2 -sensor conductivity and response on the absolute humidity of a gas mixture are given. It is shown that the relaxation time τ rel of the response of SnO 2 -and MOS-structure sensors is determined by the relaxation time τ а of hydrogen atom adsorption on the SnO 2 and SiO 2 surfaces, respectively. For the MOS-diodes, τ rel = τ а at n Н 2 <3⋅10 3 ppm and τ rel = τ d at n Н 2 ≥ 7.5⋅10 3 ppm, where τ d is the relaxation time of hydrogen atom diffusion through an SiO 2 layer.