Standard

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 изданияхстатьяРецензирование

Harvard

Ermanyuk, EV, Shmakova, ND & Flór, JB 2017, 'Internal wave focusing by a horizontally oscillating torus', Journal of Fluid Mechanics, Том. 813, стр. 695-715. https://doi.org/10.1017/jfm.2016.871

APA

Ermanyuk, E. V., Shmakova, N. D., & Flór, J. B. (2017). Internal wave focusing by a horizontally oscillating torus. Journal of Fluid Mechanics, 813, 695-715. https://doi.org/10.1017/jfm.2016.871

Vancouver

Ermanyuk EV, Shmakova ND, Flór JB. Internal wave focusing by a horizontally oscillating torus. Journal of Fluid Mechanics. 2017 февр. 25;813:695-715. doi: 10.1017/jfm.2016.871

Author

Ermanyuk, E. V. ; Shmakova, N. D. ; Flór, J. B. / Internal wave focusing by a horizontally oscillating torus. в: Journal of Fluid Mechanics. 2017 ; Том 813. стр. 695-715.

BibTeX

@article{3f5bc04186ba48d780c5eddc211fa364,
title = "Internal wave focusing by a horizontally oscillating torus",
abstract = "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.",
keywords = "Internal waves, stratified flows, topographic effects, VIBRATING ELLIPTIC CYLINDERS, DEEP-OCEAN, TOPOGRAPHY, SMALL-AMPLITUDE, STRATIFIED FLUID, internal waves, CIRCULAR-CYLINDER, PART 1, GENERATION, FLOWS, TIDAL CONVERSION",
author = "Ermanyuk, {E. V.} and Shmakova, {N. D.} and Fl{\'o}r, {J. B.}",
year = "2017",
month = feb,
day = "25",
doi = "10.1017/jfm.2016.871",
language = "English",
volume = "813",
pages = "695--715",
journal = "Journal of Fluid Mechanics",
issn = "0022-1120",
publisher = "Cambridge University Press",

}

RIS

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