Accuracy of solitary wave generation by a piston wave maker.

A new experimental procedure to generate solitary waves in a flume using a piston type wave maker is derived from Rayleigh's (1876, [18]) solitary wave solution. Resulting solitary waves fordimensionless amplitudes £ ranging from 0.05 to 0.5 are as pure as the ones generated using Goring's (1978, [7]) procedure which is based on Boussinesq (1871a, [1]) solitary wave, with trailing waves of amplitude lower than 3 % of the main pulse amplitude. In contrast with Goring's procedure, the new procedure results in very little loss of amplitude in the initial stage of the propagation of the solitary waves. We show that solitary waves generated using this new procedure are more rapidly established. This is attributed to the better description of the outskirts decay coefficient in a solitary wave given by Rayleigh's solution rather than by a Boussinesq expression. Two other generation procedures based on first-order (KdV) and second order shallow water theories are also tested. Solitary waves generated by the latter are of much lower quality than those generated with Rayleigh or Boussinesq-based procedures.

[1]  D. Clamond,et al.  Interaction between a stokes wave packet and a solitary wave , 1999 .

[2]  D. Korteweg,et al.  XLI. On the change of form of long waves advancing in a rectangular canal, and on a new type of long stationary waves , 1895 .

[3]  F. Serre,et al.  CONTRIBUTION À L'ÉTUDE DES ÉCOULEMENTS PERMANENTS ET VARIABLES DANS LES CANAUX , 1953 .

[4]  E. Barthélemy,et al.  Short wave phase shifts by large free surface solitary waves: Experiments and models , 2001 .

[5]  M. Longuet-Higgins,et al.  On the speed and profile of steep solitary waves , 1976, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[6]  D. Goring,et al.  Tsunamis -- the propagation of long waves onto a shelf , 1978 .

[7]  Michael Selwyn Longuet-Higgins,et al.  On the mass, momentum, energy and circulation of a solitary wave , 1974, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[8]  J. Boussinesq,et al.  Théorie des ondes et des remous qui se propagent le long d'un canal rectangulaire horizontal, en communiquant au liquide contenu dans ce canal des vitesses sensiblement pareilles de la surface au fond. , 1872 .

[9]  G. Whitham Linear and non linear waves , 1974 .

[10]  J. Byatt-Smith,et al.  An exact integral equation for steady surface waves , 1970, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[11]  C. Mei The applied dynamics of ocean surface waves , 1983 .

[12]  Michael Selwyn Longuet-Higgins,et al.  On the mass, momentum, energy and circulation of a solitary wave. II , 1974, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[13]  D. Renouard,et al.  Experimental study of the generation, damping, and reflexion of a solitary wave , 1985 .

[14]  M. Longuet-Higgins Trajectories of particles at the surface of steep solitary waves , 1981, Journal of Fluid Mechanics.

[15]  G. H. Keulegan Gradual damping of solitary waves , 1948 .

[16]  Costas E. Synolakis,et al.  GENERATION OF LONG WAVES IN LABORATORY , 1990 .

[17]  C. S. Gardner,et al.  Korteweg‐de Vries Equation and Generalizations. III. Derivation of the Korteweg‐de Vries Equation and Burgers Equation , 1969 .

[18]  H. Segur,et al.  The Korteweg-de Vries equation and water waves. Part 2. Comparison with experiments , 1974, Journal of Fluid Mechanics.