We show that the kinematics of gas–surface scattering has two distinctively different regions which bear consequence on the incident angle dependence of the gas/surface trapping probability. The two regions are characterized by 1−μ−2λ≳0 and 1−μ−2λ<0, where λ represents the degree of surface corrugation, and μ is the mass ratio of the gas particle to that of the effective surface scattering unit. When 1−μ−2λ≳0, the gas particles after initial scattering have a high probability of reflection. In this case, the trapping probability exhibits normal behavior, i.e., increases with an increase of the scattering angle. For the other case, the gas particles maintain a mean velocity towards the surface after the initial scattering event, and the trapping probability exhibits unusual behavior, i.e., decreases with increasing the scattering angle. A theory constructed for the latter case shows good agreement with experimental data for Cl2 molecule scattering on the Cl covered GaAs (110) surface.