Reflection and diffraction of internal solitary waves by a circular island

We have investigated the reflection and diffraction of first-mode and second-mode solitary waves by an island, using a three-dimensional nonhydrostatic numerical model. The model domain consists of a circular island 15 km in diameter in an ocean 300 m deep. We use prescribed density anomalies in an initially motionless ocean to produce highly energetic internal solitary waves; their subsequent propagation is subject to island perturbations with and without the effect of earth’s rotation. In addition to reflected waves, two wave branches pass around the island and reconnect behind it. Island perturbations to the first-mode and second-mode waves are qualitatively similar, but the latter is more profound because of the longer contact time and, in the presence of earth’s rotation, the scale compatibility between Rossby radius of the second baroclinic mode and the island diameter. Without earth’s rotation, reflected and diffracted waves are symmetrical relative to the longitudinal axis passing through the island center. With earth’s rotation, the current following the wave front veers to the right due to Coriolis deflection. For a westward propagating incoming wave, the deflection favors northward wave propagation in the region between the crossover point and the island, shifting the wave reconnection point behind the island northward. It also displaces the most visible part of the reflected waves to the southeast. In the presence of earth’s rotation, a second-mode incoming wave produces island-trapped internal Kelvin waves, which are visible after the passage of the wave front.

[1]  W. Alpers,et al.  Generation of secondary internal waves by the interaction of an internal solitary wave with an underwater bank , 2005 .

[2]  S. Chao,et al.  Effects of a baroclinic current on a sinking dense water plume from a submarine canyon and heton shedding , 2003 .

[3]  P. Liu,et al.  A two-dimensional, depth-integrated model for internal wave propagation over variable bathymetry , 2002 .

[4]  R. Fett,et al.  Satellite observation of internal wave refraction in the South China Sea , 1977 .

[5]  S. Chao,et al.  Nonhydrostatic aspects of coastal upwelling meanders and filaments off eastern ocean boundaries , 2002 .

[6]  T. Tang,et al.  Internal tide and nonlinear internal wave behavior at the continental slope in the northern south China Sea , 2004, IEEE Journal of Oceanic Engineering.

[7]  Antony K. Liu,et al.  Nonlinear Internal Waves in the South China Sea , 2000 .

[8]  K. Helfrich Internal solitary wave breaking and run-up on a uniform slope , 1992, Journal of Fluid Mechanics.

[9]  S. A. Eide,et al.  Experiments on the resonance of long-period waves near islands , 1976, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[10]  K. Hutter,et al.  Generation of second mode solitary waves by the interaction of a first mode soliton with a sill , 2001 .

[11]  Ping-Tung Shaw,et al.  A nonhydrostatic primitive-equation model for studying small-scale processes : An object-oriented approach , 2006 .

[12]  P Brandt,et al.  Structure of Large-Amplitude Internal Solitary Waves , 2000 .

[13]  Joel H. Ferziger,et al.  Introduction to Theoretical and Computational Fluid Dynamics , 1996 .

[14]  T. Tang,et al.  Solitons northeast of Tung-Sha Island during the ASIAEX pilot studies , 2004, IEEE Journal of Oceanic Engineering.

[15]  J. B. Bole,et al.  Soliton Currents In The South China Sea: Measurements And Theoretical Modeling , 1994 .