G\"ortler number-based scaling of boundary-layer transition on rotating cones in axial inflow

Abstract

This paper reports on the efficacy of the G\"ortler number in scaling the laminar-turbulent boundary-layer transition on rotating cones facing axial inflow. Depending on the half-cone angle $\psi$ and axial flow strength, the competing centrifugal and crossflow instabilities dominate the transition. Traditionally, the flow is evaluated by using two parameters: the local meridional Reynolds number $Re_l$ comparing the inertial versus viscous effects and the local rotational speed ratio $S$ accounting for the boundary-layer skew. We focus on the centrifugal effects, and evaluate the flow fields and reported transition points using G\"ortler number based on the azimuthal momentum thickness of the similarity solution and local cone radius. The results show that G\"ortler number alone dominates the late stages of transition (maximum amplification and turbulence onset phases) for a wide range of investigated $S$ and half-cone angle ($15^{\circ} \leq \psi \leq 50^{\circ}$), although the early stage (critical phase) seems to be not determined by the G\"ortler number alone on the broader cones ($\psi=30^{\circ}$ and $50^{\circ}$) where the primary crossflow instability dominates the flow. Overall, this indicates that the centrifugal effects play an important role in the boundary-layer transition on rotating cones in axial inflow.