Journal of Fluid Mechanics



On the evolution of packets of water waves


Mark J.  Ablowitz a1p1 and Harvey  Segur a2
a1 Applied Mathematics Program, Princeton University, Princeton, New Jersey 08540
a2 Aeronautical Research Associates of Princeton, Inc., 50 Washington Road, P.O. Box 2229, Princeton, New Jersey 08540

Article author query
ablowitz mj   [Google Scholar] 
segur h   [Google Scholar] 
 

Abstract

We consider the evolution of packets of water waves that travel predominantly in one direction, but in which the wave amplitudes are modulated slowly in both horizontal directions. Two separate models are discussed, depending on whether or not the waves are long in comparison with the fluid depth. These models are two-dimensional generalizations of the Korteweg-de Vries equation (for long waves) and the cubic nonlinear Schrödinger equation (for short waves). In either case, we find that the two-dimensional evolution of the wave packets depends fundamentally on the dimensionless surface tension and fluid depth. In particular, for the long waves, one-dimensional (KdV) solitons become unstable with respect to even longer transverse perturbations when the surface-tension parameter becomes large enough, i.e. in very thin sheets of water. Two-dimensional long waves (‘lumps’) that decay algebraically in all horizontal directions and interact like solitons exist only when the one-dimensional solitons are found to be unstable.

The most dramatic consequence of surface tension and depth, however, occurs for capillary-type waves in sufficiently deep water. Here a packet of waves that are everywhere small (but not infinitesimal) and modulated in both horizontal dimensions can ‘focus’ in a finite time, producing a region in which the wave amplitudes are finite. This nonlinear instability should be stronger and more apparent than the linear instabilities examined to date; it should be readily observable.

Another feature of the evolution of short wave packets in two dimensions is that all one-dimensional solitons are unstable with respect to long transverse perturbations. Finally, we identify some exact similarity solutions to the evolution equations.

(Published Online April 19 2006)
(Received May 15 1978)
(Revised September 29 1978)


Correspondence:
p1 Permanent address: Mathematics Department, Clarkson College, Potsdam, New York.


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