Skip to main content Accessibility help
×
Home
  • Get access
    Check if you have access via personal or institutional login
  • Cited by 2
  • Print publication year: 2016
  • Online publication date: February 2016

5 - A Novel Non-Local Formulation of Water Waves

Summary

Abstract

An introduction to the new formulation of the water wave problem on the basis of the unified transform is presented. The main presentation is on the three-dimensional irrotational water wave problem with surface tension forces included. Examples considered are the doubly-periodic case, the linear case, the case of a variable bottom, and the case of non-zero vorticity.

Introduction

There have been numerous important developments in the study of surface water waves that date back to the classical works of Stokes and his contemporaries in the nineteenth century. A new reformulation of this problem was presented in [1]. This reformulation is based on the so-called unified transform or the Fokas method, which provides a novel approach for the analysis of linear and integrable nonlinear boundary value problems [2, 3].

This chapter is organised as follows: section 5.2 presents the novel formulation of the 3D water waves in the case of a flat bottom. This formulation is used in section 5.3 for the derivation of the associated linearized equations as well as a 2D Boussinesq equation and the KP equation. The case of the 2D periodic water waves is discussed in section 5.4. 3D water waves in a variable bottom are discussed in section 5.5. Finally, the case of 2D water waves with constant vorticity are considered in section 5.6.

A non-local formulation governing two fluids bounded above either by a rigid lid or a free surface is presented in [4]. The case of three fluids bounded above by a rigid lid is considered in [5]. A hybrid of the novel formulation and an approach based on conformal mappings is presented in [6].

3D Water Waves with Flat Bottom

Let the domain Ωf (where the subscript f denotes flat bottom) be defined by

where η denotes the free surface of the water. One of the major difficulties of the problem of water waves is the fact that η is unknown.

Let ϕ denote the velocity potential. The two unknown functions η(x1, x2, t) and ϕ(x1, x2, y, t) satisfy the following equations:

where is the gravitational acceleration, σ and ρ denote the constant surface tension and density respectively, and h is the constant unperturbed fluid depth.

Related content

Powered by UNSILO
[1] M.J., Ablowitz, A.S., Fokas and Z.H., Musslimani, On a new non-local formulation of water waves, J. Fluid Mech., 562, 313, 2006.
[2] A.S., Fokas, A unifed transform method for solving linear and certain nonlinear PDEs, Proc. R. Soc. Lond. A, 453, 1411-1443, 1997.
[3] A.S., Fokas, A unifed approach to boundary value problems, SIAM, 78, 2008.
[4] T.S., Haut and M.J., Ablowitz, A reformulation and applications of interfacial fluids with a free surface. J. Fluid Mech., 631, 375-396, 2009.
[5] D., Burini, S., De Lillo and D., Skouteris, On a coupled system of shallow water equations admitting travelling wave solutions, submitted.
[6] A.S., Fokas and A., Nachbin, Water waves over a variable bottom: a non-local formulation and conformal mapping, J. Fluid Mech., 695, 288-309, 2012.
[7] V.E., Zakharov, Stability of periodic waves of finite amplitude on the surface of a deep fluid, J. Appl. Mech. Tech. Phys., 2, 190, 1968.
[8] W., Craig and C., Sulem, Numerical simulation of gravity waves, J. Comput. Phys., 108(1), 73-83, 1993.
[9] B., Deconinck and K., Oliveras, The instability of periodic surface gravity waves. J. Fluid Mech., 675, 141-167, 2011.
[10] D.J., Benney and J.C., Luke, Interactions of permanent waves of finite amplitude, J. Maths and Phys., 43, 455, 1964.
[11] A., Ashton and A.S., Fokas, A non-local formulation of rotational water waves, J. Fluid. Mech., 689 (1), 2011.