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3D turbulent hydrodynamics (RANS k-ω SST, RP-1 kerosene at U_in = 14.0 m/s, m = 252.4 kg/s) of a two-row rocket turbopump booster stage comprising a conical-hub 3-bladed helical inducer (pitch 34°) and a 4-vane counter-pitched deswirl stator (−18°).
High-pressure liquid rocket engine turbopumps (such as the RD-170/RD-180 and LE-7A booster pumps) place an axial helical inducer stage upstream of the main centrifugal impeller to pressurize propellant at low inlet pressure and prevent cavitation breakdown, followed by stationary deswirl stator vanes that convert tangential swirl back into axial flow. This 3D CFD model represents a Ø170 mm annular turbopump duct (420 mm length) housing a streamlined central hub that ramps radially from R_hub1 = 30 mm across the 3-bladed pitched inducer row (chord 68 mm, blade pitch +34°, 9 mm tip clearance) to R_hub2 = 42 mm across the 4-vane counter-pitched stator row (chord 52 mm, vane pitch −18°, 7 mm tip clearance). Operating on RP-1 kerosene (ρ = 800 kg/m³, μ = 0.0016 Pa·s) at U_in = 14.0 m/s (mass flow rate 252.35 kg/s), the native SU2_CFD (k-ω SST) solution resolves meridional + blade-to-blade acceleration up to |U|_max = 54.21 m/s (3.87× U_in), suction-side low-pressure pockets (−305.0 kPa) critical for NPSH cavitation screening, an axial hydrodynamic load of F_X = 11.58 kN, a stage pressure differential of Δp = 2.194 MPa, and tip-leakage vortex cores (Q_max = 4.87×10⁵ s⁻²).
Turbomachinery engineers use WebCAE CFD to screen inducer blade pitch angles, meridional hub contours, suction-side cavitation margins, and axial thrust loads on rocket turbopump bearings.
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