Lamb–Oseen vortex

Mathematical description

Oseen looked for a solution for the Navier–Stokes equations in cylindrical coordinates (r,\theta,z) with velocity components (v_r,v_\theta,v_z) of the form : v_r=0, \quad v_\theta=\frac{\Gamma}{2\pi r}g(r,t), \quad v_z=0. where \Gamma is the circulation of the vortex core. Navier–Stokes equations lead to : \frac{\partial g}{\partial t} = \nu\left(\frac{\partial^2 g}{\partial r^2} - \frac{1}{r} \frac{\partial g}{\partial r}\right) which, subject to the conditions that it is regular at r=0 and becomes unity as , leads to : g(r,t) = 1-\mathrm{e}^{-r^2/4\nu t}, where \nu is the kinematic viscosity of the fluid. At , 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 : \omega_z(r,t) = \frac{\Gamma}{4\pi \nu t} \mathrm{e}^{-r^2/4\nu t}.

The pressure field simply ensures the vortex rotates in the circumferential direction, providing the centripetal force : {\partial p \over \partial r} = \rho {v^2 \over r}, where \rho is the constant density.

Generalized Oseen vortex

The generalized Oseen vortex may be obtained by looking for solutions of the form : v_r=-\gamma(t) r, \quad v_\theta= \frac{\Gamma}{2\pi r}g(r,t), \quad v_z = 2\gamma(t) z that leads to the equation : \frac{\partial g}{\partial t} -\gamma r\frac{\partial g}{\partial r} = \nu \left(\frac{\partial^2 g}{\partial r^2} - \frac{1}{r} \frac{\partial g}{\partial r}\right).

Self-similar solution exists for the coordinate , provided , where a is a constant, in which case . The solution for \varphi(t) may be written according to Rott (1958) as : \varphi^2= 2a\exp\left(-2\int_0^t\gamma(s),\mathrm{d} s\right)\int_c^t\exp\left(2\int_0^u \gamma(s),\mathrm{d} s\right),\mathrm{d}u, where c is an arbitrary constant. For , the classical Lamb–Oseen vortex is recovered. The case \gamma=k corresponds to the axisymmetric stagnation point flow, where k is a constant. When , , a Burgers vortex is a obtained. For arbitrary , the solution becomes , where \beta is an arbitrary constant. As , Burgers vortex is recovered.

References

References

1. Oseen, C. W. (1912). Uber die Wirbelbewegung in einer reibenden Flussigkeit. Ark. Mat. Astro. Fys., 7, 14–26.
2. (1992). "Vortex dynamics". Cambridge University Press.
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.