The Kaufmann vortex, also known as the Scully model, is a mathematical model for a vortex taking account of viscosity. It uses an algebraic velocity profile. This vortex is not a solution of the Navier–Stokes equations. Kaufmann and Scully's model for the velocity in the Θ direction is:
V Θ ( r ) = Γ 2 π r r c 2 + r 2 {\displaystyle V_{\Theta }\ (r)={\frac {\Gamma }{2\pi }}{\frac {r}{r_{c}^{2}+r^{2}}}}
The model was suggested by W. Kaufmann in 1962, and later by Scully and Sullivan in 1972 at the Massachusetts Institute of Technology.
See also Rankine vortex – a simpler, but more crude, approximation for a vortex. Lamb–Oseen vortex – the exact solution for a free vortex decaying due to viscosity.
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