期刊
JOURNAL OF FLUID MECHANICS
卷 915, 期 -, 页码 -出版社
CAMBRIDGE UNIV PRESS
DOI: 10.1017/jfm.2021.179
关键词
vortex dynamics
资金
- Pawsey Supercomputer Centre under the National Computational Merit Allocation Scheme [n67, d71]
- Australian Government through the Australian Research Council's Discovery Projects funding scheme [DP170100275]
- Sir James McNeil Scholarship (SJMS)
- Monash Graduate Excellence Scholarship (MGES)
Lyman's proposed definition of the boundary vorticity flux offers conceptual benefits in describing the transfer of circulation across a boundary, extending to three-dimensional flows, and enabling control-surface analysis. The definition also illustrates how the kinematic condition of vortex lines not ending in the fluid is maintained, providing an elegant description of viscous processes like vortex reconnection. The examination of flow over a sphere using Lyman's definition demonstrates the benefits of the proposed framework in understanding vortical flow dynamics.
We examine Lyman's (App]. Mech. Rev., vol. 43, issue 8, 1990, pp. 157-158) proposed definition of the boundary vorticity flux, as an alternative to the traditional definition provided by Lighthill (Introduction: boundary layer theory. In Laminar Boundary Layers (ed. L. Rosenhead), chap. 2, 1963, pp. 46-109. Oxford University Press). While either definition may be used to describe the generation and diffusion of vorticity, Lyman's definition offers several conceptual benefits. First, Lyman's definition can be interpreted as the transfer of circulation across a boundary, due to the acceleration of that boundary, and is therefore closely tied to the dynamics of linear momentum. Second, Lyman's definition allows the vorticity creation process on a solid boundary to be considered essentially inviscid, effectively extending Morton's (Geophys. Astrophys. Fluid Dyn., vol. 28, 1984, pp. 277-308) two-dimensional description to three-dimensional flows. Third, Lyman's definition describes the fluxes of circulation acting in any two-dimensional reference surface, enabling a control-surface analysis of three-dimensional vortical flows. Finally, Lyman's definition more clearly illustrates how the kinematic condition that vortex lines do not end in the fluid is maintained, providing an elegant description of viscous processes such as vortex reconnection. The flow over a sphere, in either translational or rotational motion, is examined using Lyman's definition of the vorticity flux, demonstrating the benefits of the proposed framework in understanding the dynamics of vortical flows.
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