THE 3-DIMENSIONAL INTERACTION OF A STREAMWISE VORTEX WITH A LARGE-CHORD LIFTING SURFACE - THEORY AND EXPERIMENT

The three-dimensional vortex flow that develops around a close-coupled canard-wing configuration is characterized by a strong interaction be tween the vortex generated at the canard and the aircraft wing. In thi s paper, a theoretical potential flow model is devised to uncover the basic structure of the pressure and velocity distributions on the wing surface. The wing is modelled as a semi-infinite lifting-surface set at zero angle of attack. It is assumed that the vortex is a straight v ortex filament, with constant strength, and lying in the freestream di rection. The vortex filament is considered to be orthogonal to the lea ding-edge, passing a certain height over the surface. An incompressibl e and steady potential flow formulation is created based on the three- dimensional Laplace's equation for the velocity potential. The boundar y-value problem is solved analytically using Fourier transforms and th e Wiener-Hopf technique. A closed-form solution for the velocity poten tial is determined, from which the velocity and pressure distributions on the surface and a vortex path correction are obtained. The model p redicts an anti-symmetric pressure distribution along the span in regi on near the leading-edge, and a symmetric pressure distribution downst ream from it. The theory also predicts no vertical displacement of the vortex, but a significant lateral displacement. A set of experiments is carried out to study the main features of the flow and to test the theoretical model above. The experimental results include helium-soap bubble and oil-surface flow pattern visualization, as well as pressure measurements. The comparison shows good agreement only for a weak int eraction case, whereas for the case where the interaction is strong, s econdary boundary-layer separation and vortex breakdown are observed t o occur, mainly owing to the strong vortex-boundary layer interaction. In such a case the model does not agree well with the experiments.