“…It is difficult to explain such a behavior of transverse waves from the viewpoint of the classical detonation theory [12], where the detonation velocity is fairly definite and depends far from the detonation limits only on the physical and chemical parameters of the mixture; the detonation velocity in the gas mixture depends only weakly on the initial temperature, pressure, and density [13,14]. Hence, the process of TDW propagation in a moving and gradually mixing flow of the components is more complicated, because it involves additional physical factors in the form of nonuniform distributions of parameters of the mixture ahead of the TDW front over its height (φ, P , ρ, T , velocity v z , cross-sectional area of the mixture S c1 , etc.…”