Lamb–Oseen vortex

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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.[1][2]

Vector plot of the Lamb–Oseen vortex velocity field.
Evolution of a Lamb–Oseen vortex in air in real time. Free-floating test particles reveal the velocity and vorticity pattern. (scale: image is 20 cm wide)

Mathematical description

Oseen looked for a solution for the Navier–Stokes equations in cylindrical coordinates (r,θ,z) with velocity components (vr,vθ,vz) of the form

vr=0,vθ=Γ2πrg(r,t),vz=0.

where Γ is the circulation of the vortex core. Navier-Stokes equations lead to

gt=ν(2gr21rgr)

which, subject to the conditions that it is regular at r=0 and becomes unity as r, leads to[3]

g(r,t)=1er2/4νt,

where ν is the kinematic viscosity of the fluid. At t=0, we have a potential vortex with concentrated vorticity at the z axis; and this vorticity diffuses away as time passes. The only non-zero vorticity component is in the z direction, given by

ωz(r,t)=Γ4πνter2/4νt.

The pressure field simply ensures the vortex rotates in the circumferential direction, providing the centripetal force

pr=ρv2r,

where ρ is the constant density[4]

Generalized Oseen vortex

The generalized Oseen vortex may be obtained by looking for solutions of the form

vr=γ(t)r,vθ=Γ2πrg(r,t),vz=2γ(t)z

that leads to the equation

gtγrgr=ν(2gr21rgr).

Self-similar solution exists for the coordinate η=r/φ(t), provided φφ+γφ2=a, where a is a constant, in which case g=1eaη2/2ν. The solution for φ(t) may be written according to Rott (1958)[5] as

φ2=2aexp(20tγ(s)ds)ctexp(20uγ(s)ds)du,

where c is an arbitrary constant. For γ=0, the classical Lamb–Oseen vortex is recovered. The case γ=k corresponds to the axisymmetric stagnation point flow, where k is a constant. When c=, φ2=a/k, a Burgers vortex is a obtained. For arbitrary c, the solution becomes φ2=a(1+βe2kt)/k, where β is an arbitrary constant. As t, Burgers vortex is recovered.

See also

References

  1. Oseen, C. W. (1912). Uber die Wirbelbewegung in einer reibenden Flussigkeit. Ark. Mat. Astro. Fys., 7, 14–26.
  2. Saffman, P. G.; Ablowitz, Mark J.; J. Hinch, E.; Ockendon, J. R.; Olver, Peter J. (1992). Vortex dynamics. Cambridge: Cambridge University Press. ISBN 0-521-47739-5. p. 253.
  3. Drazin, P. G., & Riley, N. (2006). The Navier–Stokes equations: a classification of flows and exact solutions (No. 334). Cambridge University Press.
  4. G.K. Batchelor (1967). An Introduction to Fluid Dynamics. Cambridge University Press.
  5. Rott, N. (1958). On the viscous core of a line vortex. Zeitschrift für angewandte Mathematik und Physik ZAMP, 9(5-6), 543–553.