Hostname: page-component-cd9895bd7-mkpzs Total loading time: 0 Render date: 2024-12-19T00:08:11.374Z Has data issue: false hasContentIssue false

On the null-field equations for water-wave radiation problems

Published online by Cambridge University Press:  20 April 2006

P. A. Martin
Affiliation:
Department of Mathematics, University of Manchester, England

Abstract

Consider a rigid body which is performing simple harmonic oscillations of small amplitude in the free surface of deep water under gravity. Under certain geometrical conditions on ∂D, the wetted surface of the body, it is known that the linear boundary-value problem [Pscr ] for a corresponding velocity potential ϕ is uniquely solvable at all frequencies. The usual method for solving [Pscr ] is to derive a Fredholm integral equation of the second kind over ∂D. There are two familiar ways of doing this: (i) represent ϕ as a distribution of simple wave sources over ∂D, leading to an integral equation for the unknown source strength; (ii) apply Green's theorem to ϕ and a simple wave source; when the field point lies on ∂D, this gives an integral equation for the boundary values of ϕ. It is well known that both of these integral equations have unique solutions, except at the same infinite discrete set of frequencies (the irregular frequencies).

In this paper, we shall describe an alternative method for solving [Pscr ]: when the field point, in (ii), lies inside the body, we obtain an integral relation. If the simple wave source has a suitable bilinear expansion, this integral relation may be reduced to an infinite set of equations for the boundary values of ϕ. These equations, called the ‘null-field equations for water waves’, appear to be new; equations of this type were first obtained by Waterman for electromagnetic and acoustic scattering problems. The required bilinear expansion has been given by Ursell (1981) for two dimensions, and is given here for three dimensions. Using these, we show that the null-field equations always have a unique solution – irregular frequencies do not occur. This result is proved here for water waves in two and three dimensions. Similar results may be obtained for water of constant finite depth.

Type
Research Article
Copyright
© 1981 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

Erdélyi, A., Magnus, W., Oberhettinger, F. & Tricomi, F. G. 1953 Higher Transcendental Functions, vol. 2. McGraw-Hill.
Havelock, T. H. 1955 Waves due to a floating sphere making periodic heaving oscillations. Proc. R. Soc. Lond. A 231, 17.Google Scholar
John, F. 1950 On the motion of floating bodies II. Comm. Pure Appl. Math. 3, 45101.Google Scholar
Kim, W. D. 1965 On the harmonic oscillations of a rigid body on a free surface. J. Fluid Mech. 21, 427451.Google Scholar
Kleinman, R. E. & Roach, G. F. 1974 Boundary integral equations for the three-dimensional Helmholtz equation. SIAM Rev. 16, 214236.Google Scholar
Martin, P. A. 1980 On the null-field equations for the exterior problems of acoustics. Quart. J. Mech. Appl. Math. 33, 385396.Google Scholar
Mei, C. C. 1978 Numerical methods in water-wave diffraction and radiation. Ann. Rev. Fluid Mech. 10, 393416.Google Scholar
Porter, W. R. 1960 Pressure distributions, added-mass, and damping coefficients for cylinders oscillating in a free surface. Dissertation, University of California, Berkeley.
Sayer, P. 1980 An integral-equation method for determining the fluid motion due to a cylinder heaving on water of finite depth. Proc. R. Soc. Lond. A 372, 93110.Google Scholar
Thorne, R. C. 1953 Multipole expansions in the theory of surface waves. Proc. Camb. Phil. Soc. 49, 707716.Google Scholar
Ursell, F. 1949 On the heaving motion of a circular cylinder on the surface of a fluid. Quart. J. Mech. Appl. Math. 2, 218231.Google Scholar
Ursell, F. 1950 Surface waves on deep water in the presence of a submerged circular cylinder. II. Proc. Camb. Phil. Soc. 46, 153158.Google Scholar
Ursell, F. 1953 Short surface waves due to an oscillating immersed body. Proc. R. Soc. Lond. A 220, 90103.Google Scholar
Ursell, F. 1981 Irregular frequencies and the motion of floating bodies. J. Fluid Mech. 105, 143156.Google Scholar
Wang, S. 1966 The hydrodynamic forces and pressure distributions for an oscillating sphere in a fluid of finite depth. Dissertation, Massachusetts Institute of Technology.
Waterman, P. C. 1969 New formulation of acoustic scattering. J. Acoust. Soc. Am. 45, 14171429.Google Scholar
Wehausen, J. V. & Laitone, E. V. 1960 Surface waves. Handbuch der Physik, vol. 9, pp. 446778. Springer.
Yu, Y. S. & Ursell, F. 1961 Surface waves generated by an oscillating circular cylinder on shallow water: theory and experiment. J. Fluid Mech. 11, 529551.Google Scholar