The second approximation to cnoidal and solitary waves

Author:

Laitone E. V.

Abstract

The expansion method introduced by Friedrichs (1948) for the systematic development of shallow-water theory for water waves of large wavelength was used by Keller (1948) to obtain the first approximation for the finite-amplitude solitary wave of Boussinesq (1872) and Rayleigh (1876), as well as for periodic waves of permanent type, corresponding to the cnoidal waves of Korteweg & de Vries (1895).The present investigation extends Friedrich's method so as to include terms up to the fourth order from shallow-water theory for a flat horizontal bottom, and thereby obtains the complete second approximations to both cnoidal and solitary waves. These second approximations show that, unlike the first approximation, the vertical motions cannot be considered as negligible, and that the pressure variation is no longer hydrostatic.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference18 articles.

1. Friedrichs, K. O. 1948 On the derivation of the shallow water theory. Appendix to The formation of breakers and bores by J. J. Stoker.Commun. Pure Appl. Math.,1,81–5.

2. Rayleigh, Lord. 1876 On waves.Phil. Mag. (Ser. 5),1,257–79. (London, Dublin and Edinburgh.) Or (1880) Scientific Papers, 1, 252–71.

3. Stoker, J. J. 1957 Water Waves .New York:Interscience Publishers.

4. Friedrichs, K. O. & Hyers, D. H. 1954 The existence-of solitary waves.Commun. Pure Appl. Math. 7,517–50.

5. Ippen, A. T. & Kulin, G. 1955 Shoaling and breaking characteristics of the solitary wave.M.I.T., Hydrodynamics Laboratory, Technical Report, no. 15 (April).

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