“…Using the prescribed thermodynamic properties of the gas mixture and normalizing, as in [4], the sought functions, coordinates, and time (p/p 0 , ρ/ρ 0 , T /T 0 , μ/μ 0 , u/u 0 , v/u 0 , x/l, y/l, and t/t 0 ) in the equations and boundary conditions to the pressure p 0 , density ρ 0 , temperature T 0 , molecular weight μ 0 , velocity of sound u 0 = p 0 /ρ 0 , distance between the neighboring TDWs l, and time t 0 = l/u 0 , we find that the solution of the problem of continuous spin detonation depends on the following governing parameters: three dimensionless parameters in the injection system (stagnation pressure of the mixture p m /p 0 , stagnation temperature of the mixture T m /T 0 , and ratio of the total cross-sectional area of injector orifices to the total cross-sectional area of the combustor entrance S * /S c ) and four scales (total length of the combustor L, length of the cylindrical part of the combustor L c , ratio of the cross-sectional areas of the combustor exit and entrance S exit /S c , and perimeter l). The numerical study was performed for a stoichiometric mixture 2H 2 + O 2 with the following values of scaling constants: T 0 = 300 K, p 0 = 1.013·10 5 Pa, μ 0 = 12 kg/kmole, ρ 0 = p 0 m 0 /RT 0 = 0.487 kg/m 3 , and u 0 = p 0 /ρ 0 = 456 m/sec.…”