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 & 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 $A$ the oscillation amplitude and $a$ the short radius of the torus. A linear wave regime is found for $Ke<0.4$, nonlinear effects start at $Ke\approx 0.6$ 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 $\sqrt{\unicode[STIX]{x1D716}}$, with $\unicode[STIX]{x1D716}=b/a$ and $b$ is the mean radius of the torus. The relevance of wave focusing due to ocean topography is discussed.

Highlights

  • In the oceans, the interaction of the tidal motion with the bottom topography is continuously generating internal waves (Bell 1975; Vlasenko, Stashchuk & Hutter 2005; Garrett & Kunze 2007)

  • This paper presents an experimental study on internal waves emitted by a horizontally oscillating torus in a linearly stratified fluid

  • This paper considers the first experimental results on the geometric focusing of internal waves generated by a horizontally oscillating torus in a linearly stratified fluid

Read more

Summary

Introduction

The interaction of the tidal motion with the bottom topography is continuously generating internal waves (Bell 1975; Vlasenko, Stashchuk & Hutter 2005; Garrett & Kunze 2007). Bühler & Muller (2007) developed the linear theory for the oscillation of a ring with a subcritical Gaussian generatrix, and consider for the first time the effect of geometric focusing of wave energy into localized regions of high wave amplitude. Mathur & Peacock 2009), (iv) interaction of wave beams in two dimensions (Teoh, Ivey & Imberger 1997; Xing & Davies 2011; Zhang & Swinney 2014) and, as mentioned above, (v) geometric focusing by three-dimensional topography (Bühler & Muller 2007; Grisouard & Bühler 2012), recently observed near canyons (Dale & Inall 2015; Vlasenko et al 2016) These latter studies (v) are novel compared to the various types of two-dimensional focusing because of the convergence of the internal wave rays.

Theoretical considerations
Experimental set-up
Method ǫ
Data analysis and parameters
Wave pattern in XZ-plane
Comparison of measurements with linear theory
Wave pattern in XY-plane
Nonlinear effects: maximum wave amplitude and overturning
Conclusions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call