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Horseshoe vortex
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The horseshoe vortex model is a simplified representation of the system present in the flow of air around a . This vortex system is modelled by the bound vortex (bound to the wing) and two trailing vortices, therefore having a shape vaguely reminiscent of a .Millikan, Clark B., Aerodynamics of the Airplane, Figure 1.35McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Chapter 3 A is shed as the wing begins to move through the fluid. This vortex dissipates under the action of , as do the trailing vortices which eventually dissipate far behind the aircraft.

The is associated with and is a component of the system of trailing vortices.McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Chapter 4

The horseshoe vortex model is unrealistic in that it implies uniform circulation (and hence, according to the Kutta–Joukowski theorem, uniform lift) at all sections on the . 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.McCormick, Barnes W., Aerodynamics, Aeronautics, and Flight Mechanics, Figure 4.21 Nevertheless, the simpler horseshoe vortex model used with a reduced effective wingspan but same mid-plane circulation provides an adequate model for the flows induced far from the aircraft.

The term horseshoe vortex is also used in to describe the flow pattern created by strong winds 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 1973Penwarden, AD. Wise, AFE. Wind environment around buildings, cover illustration and the cause of the effect is described in contemporary wind engineering text books.Cook, NJ. The designer's guide to wind loading of building structures, Part 1, Figure 8.7

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

In nature, a horseshoe vortex can cause a to form.


Notes
  • Anderson, John D. (2007), Fundamentals of Aerodynamics, Section 5.3 (4th ed.), McGraw-Hill, New York NY.
  • L. J. Clancy (1975), Aerodynamics, Section 8.10, Pitman Publishing Limited, London
  • Cook, N.J. (1985), The designer's guide to wind loading of building structures, Part 1, Butterworths, London
  • McCormick, Barnes W., (1979), Aerodynamics, Aeronautics, and Flight Mechanics, John Wiley & Sons, Inc. New York
  • Millikan, Clark B., (1941), Aerodynamics of the Airplane, Section 1-6 John Wiley and Sons, Inc., New York
  • Penwarden, A.D., Wise, A.F.E., (1975) Wind environment around buildings, HMSO, London .
  • Piercy, N.A.V. (1944), Elementary Aerodynamics, Article 213, The English Universities Press Ltd., London.
  • Von Mises, Richard, (1959), Theory of Flight, Chapter IX - section 4, Dover Publications, Inc., New York


See also
  • Helmholtz's theorems
  • Kutta–Joukowski theorem
  • Prandtl's lifting-line model
  • Trailing vortices

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