Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
Internal wave focusing by a horizontally oscillating torus. / Ermanyuk, E. V.; Shmakova, N. D.; Flór, J. B.
в: Journal of Fluid Mechanics, Том 813, 25.02.2017, стр. 695-715.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Internal wave focusing by a horizontally oscillating torus
AU - Ermanyuk, E. V.
AU - Shmakova, N. D.
AU - Flór, J. B.
PY - 2017/2/25
Y1 - 2017/2/25
N2 - This paper presents an experimental study on internal waves emitted by a horizontally oscillating torus in a linearly stratified fluid. Two internal wave cones are generated with the kinetic energy focused at the apices of the cones above and below the torus where the wave amplitude is maximal. Their motion is measured via tracking of distortions of horizontal fluorescein dye planes created prior to the experiments and illuminated by a vertical laser sheet. The distortion of the dye planes gives a direct access to the Lagrangian displacement of local wave amplitudes and slopes, and in particular, allows us to calculate a local Richardson number. In addition particle image velocimetry measurements are used. Maximum wave slopes are found in the focal region and close to the surface of the torus. As the amplitude of oscillations of the torus increases, wave profiles in the regions of maximum wave slopes evolve nonlinearly toward local overturning. A theoretical approximation based on the theory of Hurley and Keady (J. Fluid Mech., vol. 351, 1997, pp. 119-138) is presented and shows, for small amplitudes of oscillation, a very reasonable agreement with the experimental data. For the focal region the internal wave amplitude is found to be overestimated by the theory. The wave breaking in the focal region is investigated as a function of the Keulegan-Carpenter number, Ke = A/a , with the oscillation amplitude and the short radius of the torus. A linear wave regime is found for Ke < 0.4 nonlinear effects start at Ke ≈ 0.6 and breaking for ke < 0.8. For large forcing, the measured wave amplitude normalized with the oscillation amplitude decreases almost everywhere in the wave field, but increases locally in the focal region due to nonlinear effects. Due to geometric focusing the amplitude of the wave increases with ϵ with ϵ = b/a and b is the mean radius of the torus. The relevance of wave focusing due to ocean topography is discussed.
AB - This paper presents an experimental study on internal waves emitted by a horizontally oscillating torus in a linearly stratified fluid. Two internal wave cones are generated with the kinetic energy focused at the apices of the cones above and below the torus where the wave amplitude is maximal. Their motion is measured via tracking of distortions of horizontal fluorescein dye planes created prior to the experiments and illuminated by a vertical laser sheet. The distortion of the dye planes gives a direct access to the Lagrangian displacement of local wave amplitudes and slopes, and in particular, allows us to calculate a local Richardson number. In addition particle image velocimetry measurements are used. Maximum wave slopes are found in the focal region and close to the surface of the torus. As the amplitude of oscillations of the torus increases, wave profiles in the regions of maximum wave slopes evolve nonlinearly toward local overturning. A theoretical approximation based on the theory of Hurley and Keady (J. Fluid Mech., vol. 351, 1997, pp. 119-138) is presented and shows, for small amplitudes of oscillation, a very reasonable agreement with the experimental data. For the focal region the internal wave amplitude is found to be overestimated by the theory. The wave breaking in the focal region is investigated as a function of the Keulegan-Carpenter number, Ke = A/a , with the oscillation amplitude and the short radius of the torus. A linear wave regime is found for Ke < 0.4 nonlinear effects start at Ke ≈ 0.6 and breaking for ke < 0.8. For large forcing, the measured wave amplitude normalized with the oscillation amplitude decreases almost everywhere in the wave field, but increases locally in the focal region due to nonlinear effects. Due to geometric focusing the amplitude of the wave increases with ϵ with ϵ = b/a and b is the mean radius of the torus. The relevance of wave focusing due to ocean topography is discussed.
KW - Internal waves
KW - stratified flows
KW - topographic effects
KW - VIBRATING ELLIPTIC CYLINDERS
KW - DEEP-OCEAN
KW - TOPOGRAPHY
KW - SMALL-AMPLITUDE
KW - STRATIFIED FLUID
KW - internal waves
KW - CIRCULAR-CYLINDER
KW - PART 1
KW - GENERATION
KW - FLOWS
KW - TIDAL CONVERSION
UR - http://www.scopus.com/inward/record.url?scp=85010878071&partnerID=8YFLogxK
U2 - 10.1017/jfm.2016.871
DO - 10.1017/jfm.2016.871
M3 - Article
AN - SCOPUS:85010878071
VL - 813
SP - 695
EP - 715
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
SN - 0022-1120
ER -
ID: 10313613