Rankine Vortex
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The Rankine vortex is a simple mathematical model of a
vortex In fluid dynamics, a vortex (: vortices or vortexes) is a region in a fluid in which the flow revolves around an axis line, which may be straight or curved. Vortices form in stirred fluids, and may be observed in smoke rings, whirlpools in th ...
in a
viscous Viscosity is a measure of a fluid's rate-dependent resistance to a change in shape or to movement of its neighboring portions relative to one another. For liquids, it corresponds to the informal concept of ''thickness''; for example, syrup h ...
fluid. It is named after its discoverer,
William John Macquorn Rankine William John Macquorn Rankine (; 5 July 1820 – 24 December 1872) was a Scottish mathematician and physicist. He was a founding contributor, with Rudolf Clausius and William Thomson (Lord Kelvin), to the science of thermodynamics, particularl ...
. The vortices observed in nature are usually modelled with an
irrotational In vector calculus, a conservative vector field is a vector field that is the gradient of some function. A conservative vector field has the property that its line integral is path independent; the choice of path between two points does not chan ...
(potential or free) vortex. However, in a potential vortex, the velocity becomes infinite at the vortex center. In reality, very close to the origin, the motion resembles a solid body rotation. The Rankine vortex model assumes a solid-body rotation inside a cylinder of radius a and a potential vortex outside the cylinder. The radius a is referred to as the vortex-core radius. The velocity components (v_r,v_\theta,v_z) of the Rankine vortex, expressed in terms of the cylindrical-coordinate system (r,\theta,z) are given by :v_r=0,\quad v_\theta(r) = \frac\begin r/a^2 & r \le a, \\ 1/ r & r > a \end, \quad v_z = 0 where \Gamma is the circulation strength of the Rankine vortex. Since solid-body rotation is characterized by an azimuthal velocity \Omega r, where \Omega is the constant
angular velocity In physics, angular velocity (symbol or \vec, the lowercase Greek letter omega), also known as the angular frequency vector,(UP1) is a pseudovector representation of how the angular position or orientation of an object changes with time, i ...
, one can also use the parameter \Omega =\Gamma/(2\pi a^2) to characterize the vortex. The
vorticity In continuum mechanics, vorticity is a pseudovector (or axial vector) field that describes the local spinning motion of a continuum near some point (the tendency of something to rotate), as would be seen by an observer located at that point an ...
field (\omega_r,\omega_\theta,\omega_z) associated with the Rankine vortex is :\omega_r=0,\quad \omega_\theta=0, \quad \omega_z = \begin 2\Omega & r \le a, \\ 0 & r > a \end. At all points inside the core of the Rankine vortex, the vorticity is uniform at twice the angular velocity of the core; whereas vorticity is zero at all points outside the core because the flow there is irrotational. In reality, vortex cores are not always circular; and vorticity is not exactly uniform throughout the vortex core.


See also

* Burgers vortex * Kaufmann (Scully) vortex – an alternative mathematical simplification for a vortex, with a smoother transition. * Lamb–Oseen vortex – the exact solution for a free vortex decaying due to viscosity.


References


External links


Streamlines vs. Trajectories in a Translating Rankine Vortex
an example of a Rankine vortex imposed on a constant velocity field, with animation. Equations of fluid dynamics Vortices {{math-stub