This study documents a process to design a rocket based ejector nozzle propulsion system for use on a small, winged aircraft. Ejector nozzles offer a possibility to address system design problems associated with a rocket propelled aircraft; the need to address base and/or boattail drag at supersonic speeds, the need for a large propellant tank but relatively small nozzle and the need for high specific impulse particularly at subsonic and transonic speeds flown within the troposphere. We incorporated Bernstein's Compound Compressible Flow Theory into an improved ejector design method. Using this approach, we have developed and documented a numerical procedure to compute the geometry of a high-performance ejector optimized to specific flight conditions.
Nomenclaturea D = Diffuser Area Ratio a E = Secondary to Primary Inlet Area Ratio A = Area b = Wing Span C p = Coefficient of Pressure = (P-P )/q ̅̅̅ = Canonical Pressure Coefficient (C p normalized to =1 at minimum suction, =0 at trailing edge) C D = Coefficient of Drag (referenced to the maximum body diameter) D = Drag Isp = Specific Impulse (sec) ̇ = Mass Flow M = Mach Number M e = Exit Mach Number P = Static Pressure P = Differential Pressure q = Dynamic Pressure Re = Reynolds Number S = Stratford / AMO Smith Separation Criterion S = Maximum Body Cross Sectional Area Sbase = Base Area T = Thrust V e = Rocket Exit Velocity V P = Primary Stream Velocity V S = Secondary Stream Velocity x = Axial Location β = Compound Compressible Flow Indicator = Density γ = Ratio of Specific Heats ϕ = Thrust Augmentation Ratio