Hostname: page-component-cd9895bd7-dzt6s Total loading time: 0 Render date: 2024-12-28T22:26:23.865Z Has data issue: false hasContentIssue false

On the reflection of a train of finite-amplitude internal waves from a uniform slope

Published online by Cambridge University Press:  21 April 2006

S. A. Thorpe
Affiliation:
Institute of Oceanographic Sciences, Wormley, Godalming, Surrey, UK Present address: Department of Oceanography, The University, Southampton SO9 5NH, UK.
S. A. Thorpe
Affiliation:
Institute of Oceanographic Sciences, Wormley, Godalming, Surrey, UK
A. P. Haines
Affiliation:
Institute of Oceanographic Sciences, Wormley, Godalming, Surrey, UK

Abstract

The reflection of a train of two-dimensional finite-amplitude internal waves propagating at an angle β to the horizontal in an inviscid fluid of constant buoyancy frequency and incident on a uniform slope of inclination α is examined, specifically when β > α. Expressions for the stream function and density perturbation are derived to third order by a standard iterative process. Exact solutions of the equations of motion are chosen for the incident and reflected first-order waves. Whilst these individually generate no harmonics, their interaction does force additional components. In addition to the singularity at α = β when the reflected wave propagates in a direction parallel to the slope, singularities occur for values of α and β at which the incident-wave and reflected-wave components are in resonance; strong nonlinearity is found at adjacent values of α and β. When the waves are travelling in a vertical plane normal to the slope, resonance is possible at second order only for α < 8.4° and β < 30°. At third order the incident wave is itself modified by interaction with reflected components. Third-order resonances are only possible for α < 11.8° and, at a given α, the width of the β-domain in which nonlinearities connected to these resonances is important is much less than at second order. The effect of nonlinearity is to reduce the steepness of the incident wave at which the vertical density gradient in the wave field first becomes zero, and to promote local regions of low static stability remote from the slope. The importance of nonlinearity in the boundary reflection of oceanic internal waves is discussed.

In an Appendix some results of an experimental study of internal waves are described. The boundary layer on the slope is found to have a three-dimensional structure.

Type
Research Article
Copyright
© 1987 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Baines, P. G. 1971 The reflexion of internal/inertial waves from bumpy surfaces. J. Fluid Mech. 46, 273291.Google Scholar
Cacchione, D. & Wunsch, C. 1974 Experimental study of internal waves over a slope. J. Fluid Mech. 66, 223240.Google Scholar
Eriksen, C. C. 1982 Observations of internal wave reflection off sloping bottoms. J. Geophys. Res. 87, 525538.Google Scholar
Eriksen, C. C. 1985 Implications of ocean bottom reflection for internal wave spectra and mixing. J. Phys. Oceanogr. 15, 11451156.Google Scholar
Garrett, C. 1979 Mixing in the ocean interior. Dyn. Atmos. Oceans, 3, 239265.Google Scholar
Garrett, C. & Munk, W. 1972 Oceanic mixing by breaking internal waves. Deep-Sea Res. 19, 823832.Google Scholar
GÖrtler, H. 1943 Uber eine Schwingungerscheinung in Flussigkeiten mit stabiler Dichteschichtung. Z. Angew. Math. Mech. 23, 6571.Google Scholar
Hart, J. E. 1971 A possible mechanism for boundary layer mixing and layer formation in a stratified fluid. J. Phys. Oceanogr. 1, 258262.Google Scholar
Mcewan, A. D. 1971 Degeneration of resonantly-excited standing internal gravity waves. J. Fluid Mech. 50, 431448.Google Scholar
Mcewan, A. D., Mander, D. W. & Smith, R. K. 1972 Forced resonant second-order interaction between damped internal waves. J. Fluid Mech. 53, 589608.Google Scholar
Martin, S., Simmons, W. F. & Wunsch, C. I. 1972 The excitation of resonant triads by single internal waves. J. Fluid Mech. 53, 1744.Google Scholar
Mied, R. P. 1976 The occurrence of parametric instability in finite-amplitude internal gravity waves. J. Fluid Mech. 78, 763784.Google Scholar
Mied, R. P. & Dugan, J. P. 1976 Internal wave reflexion from a sinusoidally corrugated surface. J. Fluid Mech. 76, 259272.Google Scholar
Mowbray, D. E. & Rarity, B. S. H. 1967 A theoretical and experimental investigation of internal waves of small amplitude in a density stratified liquid. J. Fluid Mech. 28, 116.Google Scholar
Munk, W. H. 1966 Abyssal recipes. Deep-Sea Res. 13, 207230.Google Scholar
Phillips, O. M. 1966 The Dynamics of the Upper Ocean. Cambridge University Press. 261 pp.
Phillips, O. M. 1970 On flows induced by diffusion in a stably stratified fluid. Deep-Sea Res. 17, 435443.Google Scholar
Simpson, J. E. 1972 Effects of the lower boundary on the head of a gravity current. J. Fluid Mech. 53, 759768.Google Scholar
Thorpe, S. A. 1968 On the shape of progressive internal waves. Phil. Trans. R. Soc. Lond. A263, 563614.Google Scholar
Thorpe, S. A. 1978 On internal gravity waves in an accelerating shear flow. J. Fluid Mech. 88, 623639.Google Scholar
Thorpe, S. A. 1982 On the layers produced by rapidly oscillating a vertical grid in a uniformly stratified fluid. J. Fluid Mech. 124, 391409.Google Scholar
Thorpe, S. A. 1987 Transitional phenomena and the development of turbulence in stratified fluids: a review. J. Geophys. Res. (to appear).Google Scholar
Turner, J. S. 1973 Buoyancy Effects in Fluids. Cambridge University Press. 367 pp.
Wunsch, C. 1969 Progressive internal waves on slopes. J. Fluid Mech. 35, 131144.Google Scholar
Wunsch, C. 1970 On oceanic boundary mixing. Deep-Sea Res. 17, 293301.Google Scholar
Wunsch, C. 1971 Note on some Reynolds stress effects of internal waves on slopes. Deep-Sea Res. 18, 583591.Google Scholar