Jet group: Difference between revisions

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m Dating maintenance tags: {{Unreferenced}}
Clarified that R^* means the dual of R
 
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The Kaufmann vortex, also known as the Scully model,<ref name=umd>Mahendra J. Bhagwat and J. Gordon Leishman, [http://www.enae.umd.edu/~leishman/Aero/AHS2002_Bhagwat.pdf Generalized Viscous Vortex Model for Application to Free-Vortex Wake and Aeroacoustic Calculations], University of Maryland</ref> is a [[mathematical model]] for a [[vortex]] taking account of [[viscosity]]. It uses an algebraic velocity profile.<ref>Tamás Gausz, Budapest University of Technology and Economics. [http://rht.bme.hu/letoltesek/Dr.Gausz%20Tamas%20anyagai/Cmff/Blade%20Vortex%20Interaction%20Problems%20at%20Helicopter%20Rotors.pdf Blade vortex interaction problem at helicopter rotors], 12th International Conference on Fluid Flow Technologies, 2003</ref>
 
Kaufmann and Scully's model for the [[velocity]] in the Θ direction is:
 
:<math>V_\Theta\ (r) = \frac{\Gamma}{2\pi} \frac{r}{r_c^2 + r^2} </math>
 
The model was suggested by Scully and Sullivan in 1972 at [[Massachusetts Institute of Technology]], and earlier by W. Kaufmann in 1962.<ref>See citations 19 and 20 in Bhagwat and Leishman's paper.</ref>
 
==References==
{{Reflist}}
 
{{DEFAULTSORT:Kaufmann (Scully) Vortex}}
[[Category:Equations of fluid dynamics]]
[[Category:Vortices]]
 
 
{{Fluiddynamics-stub}}

Latest revision as of 22:52, 8 July 2014

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