Horseshoe vortex

A horseshoe vortex caused by a (purely theoretical) uniform lift distribution over an aircraft’s wing
Any change in lift distribution sheds a new trailing vortex, according to the lifting-line theory
A realistic lift distribution causes the shedding of a complex vorticity pattern behind the aircraft.

The horseshoe vortex model is a simplified representation of the vortex system of a wing. In this model the wing vorticity is modelled by a bound vortex of constant circulation, travelling with the wing, and two trailing wingtip vortices, therefore having a shape vaguely reminiscent of a horseshoe.[1][2] A starting vortex is shed as the wing begins to move through the fluid, which dissipates under the action of viscosity,[3] as do the trailing vortices far behind the aircraft.

The trailing wingtip vortices are responsible for the component of the downwash which creates induced drag.[4]

The horseshoe vortex model is unrealistic in that it implies a constant circulation (and hence, according to the Kutta–Joukowski theorem, constant lift) at all sections on the wingspan. In a more realistic model, the lifting-line theory, the vortex strength varies along the wingspan, and the loss in vortex strength is shed as a vortex-sheet all along the trailing edge, rather than as a single trail at the wing-tips.[5] Nevertheless, the simpler horseshoe vortex model used with a reduced effective wingspan but same midplane circulation provides an adequate model for the flows induced far from the aircraft.

The term horse-shoe vortex is also used in Wind Engineering to describe the vortex of strong winds that form around the base of a tall building. This effect is amplified by the presence of a low-rise building just upwind. This effect was studied at the UK Building Research Establishment between 1963 and 1973[6] and the cause of the effect is described in contemporary wind engineering text books.[7]

In hydrodynamics, a form of horseshoe vortex forms around bluff bodies in the flowing water, for instance around bridge piers.[8] They can cause scouring of bed materials from both upstream and downstream of the pier.

References

Notes

  1. ↑ Millikan, Clark B., Aerodynamics of the Airplane, Figure 1.35
  2. ↑ McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Chapter 3
  3. ↑ "Shed Vortex". NASA Glenn Research Center. Retrieved April 11, 2015.
  4. ↑ McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Chapter 4
  5. ↑ McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Figure 4.21
  6. ↑ Penwarden, AD. Wise, AFE. Wind environment around buildings, cover illustration
  7. ↑ Cook, NJ. The designer's guide to wind loading of building structures, Part 1, Figure 8.7
  8. ↑ Dargahi, Bijan (1989). "The turbulent flow field around a circular cylinder". Experiments in Fluids. Retrieved 2016-04-22.

See also

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