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In
fluid dynamics In physics and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids—liquids and gases. It has several subdisciplines, including '' aerodynamics'' (the study of air and other gases in motion) ...
, Batchelor vortices, first described by
George Batchelor George Keith Batchelor FRS (8 March 1920 – 30 March 2000) was an Australian applied mathematician and fluid dynamicist. He was for many years a Professor of Applied Mathematics in the University of Cambridge, and was founding head of the D ...
in a 1964 article, have been found useful in analyses of airplane vortex wake hazard problems.


The model

The Batchelor vortex is an approximate solution to the
Navier–Stokes equations In physics, the Navier–Stokes equations ( ) are partial differential equations which describe the motion of viscous fluid substances, named after French engineer and physicist Claude-Louis Navier and Anglo-Irish physicist and mathematician G ...
obtained using a
boundary layer In physics and fluid mechanics, a boundary layer is the thin layer of fluid in the immediate vicinity of a bounding surface formed by the fluid flowing along the surface. The fluid's interaction with the wall induces a no-slip boundary cond ...
approximation. The physical reasoning behind this approximation is the assumption that the axial gradient of the flow field of interest is of much smaller magnitude than the radial gradient.
The axial, radial and azimuthal velocity components of the vortex are denoted U,V and W respectively and can be represented in cylindrical coordinates (x,r, \theta) as follows:
: \begin U(r) &= U_\infty + \frac e^, \\ V(r) &= 0, \\ W(r) &= qW_0 \frac. \end The parameters in the above equations are * U_\infty, the free-stream axial velocity, * W_0, the velocity scale (used for nondimensionalization), * R_0, the length scale (used for nondimensionalization), * R = R(t) = \sqrt, a measure of the core size, with initial core size R_0 and \nu representing viscosity, * q, the swirl strength, given as a ratio between the maximum tangential velocity and the core velocity.
Note that the radial component of the velocity is zero and that the axial and azimuthal components depend only on r.
We now write the system above in dimensionless form by scaling time by a factor R_0/W_0. Using the same symbols for the dimensionless variables, the Batchelor vortex can be expressed in terms of the dimensionless variables as
: \left\lbrace \begin U(r) &= a + \displaystyle, \\ V(r) &= 0, \\ W(r) &= q \displaystyle, \end\right. where a = U_\infty/W_0 denotes the free stream axial velocity and Re is the Reynolds number. If one lets a = 0 and considers an infinitely large swirl number then the Batchelor
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 t ...
simplifies to the
Lamb–Oseen vortex In fluid dynamics, the Lamb–Oseen vortex models a line vortex that decays due to viscosity. This vortex is named after Horace Lamb and Carl Wilhelm Oseen. Mathematical description Oseen looked for a solution for the Navier–Stokes equa ...
for the azimuthal velocity: :W_\Theta(r) = \frac \left ( 1-e^ \right ) where \Gamma is the circulation.


References


External links


Continuous spectra of the Batchelor vortex
(Authored by Xueri Mao and Spencer Sherwin and published by
Imperial College London Imperial College London (legally Imperial College of Science, Technology and Medicine) is a public research university in London, United Kingdom. Its history began with Prince Albert, consort of Queen Victoria, who developed his vision for a ...
) Equations of fluid dynamics Vortices Fluid dynamics {{Fluiddynamics-stub