期刊
PHYSICAL REVIEW FLUIDS
卷 5, 期 10, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevFluids.5.103801
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资金
- Office of Naval Research [N00014-11-1-0511]
- National Science Foundation OCE CAREER Grant [0845558]
- National Science Foundation OCE Grant [1634257]
- Directorate For Geosciences
- Division Of Ocean Sciences [0845558] Funding Source: National Science Foundation
- Division Of Ocean Sciences
- Directorate For Geosciences [1634257] Funding Source: National Science Foundation
The development of a separated bottom boundary layer in the footprint of a large-amplitude internal solitary wave of depression, propagating against an oncoming barotropic current, is examined in detail using high-resolution implicit large eddy simulation. The wave is supported by a continuous two-layer stratification. The Reynolds number based on the water column height is 1.6 x 10(5). This numerical simulation is the first to reproduce the self-sustained three-dimensional vortex shedding, resultant transition, and turbulence under an ISW, which have long been hypothesized to occur in field experiments. No artificial noise is inserted into the flow domain. Part I of this study focuses on a structural description of the sequence of flow regimes developing from a wave-induced, long, high-aspect-ratio, laminar separation bubble. Three illuminating topological features are identified. (a) The spatial development of the self-sustained turbulence is composed of three transitional stages: (i) spontaneous excitation of a global instability in the separation bubble that emanates trailing vortices, (ii) vortex breakup and degeneration into turbulent clouds, and (iii) relaxation to a spatially developing turbulent boundary layer. (b) In the separation bubble, there exists a three-dimensional linear global oscillator, which is primarily excited by the two-dimensional absolute instability of the separated shear layer. This global mode possesses a transverse coherent structure. The transverse perturbation subsequently excites an elliptic instability mode inside the shed vortex, resulting in an axial distortion of the vortex core. (c) A shortwave secondary instability is excited in the form of a series of coherent streamwise vortex streaks that wrap around each shed vortex, leading to rapid break up and burst of the vortex.
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