A stereoscopic PIV study on the behavior of near-field wingtip vortex structures
نویسندگان
چکیده
Wingtip vortex flow is of great importance because of its effect on practical problems such as landing separation distances for aircraft, blade/vortex interactions on helicopter blades, and propeller cavitations on ships. Extensive investigations have been conducted to improve the understanding of the tip vortex structure and its dissipation or persistence analytically, numerically, and experimentally. The universal feature of the water/wind tunnel generated wing tip vortex reported in the past is vortex wandering – the slow side-to-side movement of the wing-tip vortex core behind the wing. Thus, a primary result of wandering is that fixed probe measurements of velocity and pressure cannot be trusted at distances more than one chord downstream of the wing. For reliable data, the current study investigates the behavior and structure of the near-field wing-tip vortex generated by a square-tipped, rectangular NACA0012 wing by using the stereoscopic Particle Image Velocimetry (SPIV) technique. SPIV is a spatially resolved, instantaneous, three velocity component non-intrusive measurement technique used to conserve the three key feature of the wing-tip vortex during the measurement – small vortex core dimension, core structure, and strong unsteadiness of the core flow, which wasn’t possible with classical instrumentations. One of the great advantages of SPIV over the classical technique is that the vortex wandering can be removed by tracking the center of the vortex in every SPIV frame. By tracking the center of the vortex, the wandering and turbulence in the vortex can be separated. The results show that after re-centering the velocity field, the T.K.E. and Reynolds stress distributions become lower by more than twice at 4.0c downstream.
منابع مشابه
On Coherent Structures of Turbulent Open-channel Flow Above a Rough Bed
Present study examines turbulent structures of a rough bed open-channel flow in the context of deterministic approach. Instantaneous velocity field is measured in different hydraulic conditions using two dimensional Particle Image Velocimetry (PIV) in vertical plane and Stereoscopic PIV in horizontal plane. Different techniques and quantities such as swirl strength, two-point and cross-correlat...
متن کاملApplication of Wavelet Vector Multi-resolution Technique to Piv Measurements
A wavelet-based vector multi-resolution technique was applied to analyze the three-dimensional measurement results of a high-resolution stereoscopic PIV system in this paper. The instantaneous threedimensional flow structures in the near field of lobed jet mixing flow were successfully decomposed into largeand small-scale structures based on the wavelet vector multi-resolution analysis. It is f...
متن کاملPhase-averaged scanning stereoscopic PIV measurement for classification of vortex regime of synthetic jet in cross flow
A synthetic jet is one of flow control devices that can topologically disturb surrounding flow field by adding periodic injection and suction of surrounding fluid using an oscillating membrane through an orifice. This device can be applied to the downsized fluid machinery without a net mass injection of fluid for the simplified structure. In this study, the phase-averaged three-dimensional flow...
متن کاملEvaluating the effects of near-field earthquakes on the behavior of moment resisting frames
Following the 1994 Northridge and 1995 Kobe earthquakes, most of modern structures damaged seriously or devastated totally despite the seismic codes of these countries that had been expected to bear advanced criteria for seismic design of structures. After extensive research, the most probable reason of those destructions was attributed to special specifications of near-field earthquakes. In th...
متن کاملStructure Identification and Analysis in Turbulent Boundary Layers by Stereo PIV
Stereoscopic PIV was used to measure three instantaneous components of velocity in streamwisespanwise planes of a turbulent boundary layer. The local boundary layer thickness was δ = 69 mm, and the corresponding Reynolds number based on friction velocity was 1060. Data sets were obtained in the log region at wall-normal positions of z = 92 and z = 192. The resulting velocity fields at z = 92 re...
متن کامل