2026-05-27T05:24:57Zhttps://riuma.uma.es/rest/oai/requestoai:riuma.uma.es:10630/376082026-02-03T12:06:34Zcom_10630_2254col_10630_37959
RIUMA. Repositorio Institucional de la Universidad de Málaga
author
Durán Venegas, Eduardo
author
Le Dizès, Stéphane
2025-02-03T10:06:34Z
2025-02-03T10:06:34Z
2018
12th European Fluid Mechanics Conference, 2018. Viena (Austria)
https://hdl.handle.net/10630/37608
We study the structure and stability of the vortical wake generated by a two-blade Joukowski rotor of radius Rb, rotating at angular velocity ⌦ in an axial wind of velocity V1. In this rotor model, each blade is assumed to emit a free tip vortex of circulation and a hub vortex of opposite circulation centered on the rotor axis. Considering a fixed vortex core size a and neglecting viscosity, the vortex dynamics is computed by a free vortex method1 using the Biot-Savart law.
The problem is defined by three non-dimensionalized parameters: the tip speed ratio = Rb⌦/V1, the vortex strength ⌘ = /⌦Rb2 and the vortex thickness " = a/Rb. For a small and fixed vortex thickness " = 0.01, we first show that stationary solutions (in the rotating frame) can be obtained for almost all values of and ⌘ except in a small parameter region indicated in gray in figure 1(a). In this figure are indicated the di↵erent flight regimes of a helicopter associated with each solution. Of particular interest is the so-called Vortex Ring State (VRS) occurring during rapid descent that cannot be described by the general momentum theory2. In this regime, vortices are present on both sides of the rotor plane as illustrated in figure 1(b).
The stability of the various solutions is also addressed by analyzing the linear response to a Dirac perturbation applied at the rotor tip. For most flight regimes, the flow is found to be convectively unstable: the perturbation grows but is advected away from the rotor plane. The property of the wave packet far away has been compared to the theoretical predictions for uniform helices3 and a very good agreement has been observed [see figure 1(c)]. In the VRS regime, a di↵erent behavior is observed: the perturbation continues to grow in the neighborhood of the rotor and a well-defined global mode emerges everywhere. The rotor wake has become globally unstable.
eng
Atribución-NoComercial-CompartirIgual 4.0 Internacional
Movimiento de vórtices
Structure and stability of rotor generated vortices
conference output
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