Bulletin of the American Physical Society
77th Annual Meeting of the Division of Fluid Dynamics
Sunday–Tuesday, November 24–26, 2024; Salt Lake City, Utah
Session A38: Vortex Dynamics and Vortex Flows: Fundamentals
8:00 AM–10:10 AM,
Sunday, November 24, 2024
Room: 355 D
Chair: Bartosz Protas, McMaster University
Abstract: A38.00009 : Kelvin wave exchange between toroidal vortices*
9:44 AM–9:57 AM
Presenter:
Oscar U Velasco Fuentes
(CICESE)
Authors:
Manuel S Antonio Pérez
(CICESE)
Oscar U Velasco Fuentes
(CICESE)
in an incompressible inviscid fluid. The vortices are thin tubes of equal
cross-section and circulation. The helico-toroidal vortex lies on the surface
of an immaterial torus (radius: r0, cross sectional radius: r1) and is
characterised by the number of turns, q, that it makes round the torus
centerline while making one turn round the torus symmetry axis to close
on itself. The vortex ring and the immaterial torus have the same
centerline. Under these initial conditions, the flow evolution depends only
on q, r1/r0 and a (the cross-sectional radius of the vortices). Numerical
simulations using the Rosenhead-Moore approximation to the Biot-Savart
law show that for small r1/r0 (<0.2) the vortices translate along and rotate
around the torus symmetry axis while changing shape almost periodically:
at regular intervals the helico-toroidal vortex becomes an almost circular
vortex ring and vice versa. The linear speed of the vortices decreases and
their angular speed increases with growing values of the parameters q and
r1/r0. The capacity of the vortices to carry fluid decreases while their
capacity to stir their surroundings increases as r1/r0 increases.
*Supported by Conahcyt (Mexico) through a post-graduate scholarship to MAP.
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