Hostname: page-component-cd9895bd7-hc48f Total loading time: 0 Render date: 2024-12-23T10:57:16.040Z Has data issue: false hasContentIssue false

A cylindrical wave-maker problem in a liquid of finite depth with an inertial surface in the presence of surface tension

Published online by Cambridge University Press:  17 February 2009

N. K. Ghosh
Affiliation:
Department of Applied Mathematics, Calcutta University, Calcutta-700009, India.
Rights & Permissions [Opens in a new window]

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

The problem of generation of waves in a liquid of uniform finite depth with an inertial surface composed of a thin but uniform distribution of disconnected floating particles, due to forced axisymmetric motion prescribed on the surface of an immersed vertical cylindrical wave-maker of circular cross section under the influence of surface tension at the inertial surface, is discussed. The techniques of Laplace transform in time and the modified Weber transform involving Bessel functions in the radial coordinate have been employed to obtain the velocity potential. The steady-state development to the potential function as well as the inertial surface depression due to time-harmonic forced oscillations of the wave-maker are deduced. It is found that the presence of surface tension at the inertial surface ensures the propagation of time-harmonic progressive waves of any angular frequency.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 1991

References

[1]Evans, D. V., “The influence of surface tension on the reflection of water waves by a plane vertical barrier”, Proc. Camb. Phil. Soc. 64 (1968) 795810.CrossRefGoogle Scholar
[2]Evans, D. V., “The effect of surface tension on the waves produced by a heaving circular cylinder”, Proc. Camb. Phil. Soc. 64 (1968) 833847.CrossRefGoogle Scholar
[3]Havelock, T. H., “Forced surface waves on water”, Phil. Mag. 8 (1929) 569576.CrossRefGoogle Scholar
[4]Hocking, L. M., “Capillary-gravity waves produced by a heaving body”, J. Fluid Mech. 186 (1988) 337349.CrossRefGoogle Scholar
[5]Mandal, B. N., “A note on the Havelock's cylindrical wave-maker problems”, Rev. Roum. Sci. Techn.-Mec. Appl. 34 (1989) 185190.Google Scholar
[6]Mandal, B. N. and Kundu, K., “A note on the singularities in the theory of water waves with an inertial surface”, J. Austral. Math. Soc. Ser. B28 (1986) 271278.CrossRefGoogle Scholar
[7]Mandal, B. N. and Kundu, K., “A note on the cylindrical wavemaker problem in a liquid with an inertial surface,” Int. J. Engng. Sci. 27 (1989) 393398.CrossRefGoogle Scholar
[8]Mandal, B. N. and Kundu, K., “A cylindrical wave-maker problem in a liquid of finite depth with an inertial surface”, Indian J. Pure and Appl. Math. 20 (1989) 505512.Google Scholar
[9]Rhodes-Robinson, P. F., “On the forced surface waves due to a vertical wave-maker in the presence of surface tension”, Proc. Camb. Phil. Soc. 70 (1971) 323337.CrossRefGoogle Scholar
[10]Rhodes-Robinson, P. F., “On the generation of water waves at an inertial surface,” J. Austral. Math. Soc. Ser. B25 (1984) 366383.CrossRefGoogle Scholar
[11]Rhodes-Robinson, P. F., “Note on the effect of surface tension on water waves at an inertial surface”, J. Fluid Mech. 125 (1982) 375377.CrossRefGoogle Scholar
[12]Titchmarsh, E. C., Eigenfunction expansions associated with second order differential equations, (Oxford University Press, 1962, p. 87).Google Scholar