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Gravity–capillary rings generated by water drops

Published online by Cambridge University Press:  21 April 2006

Bernard Le Méhauté
Affiliation:
Division of Applied Marine Physics, Rosenstiel School of Marine and Atmospheric Science, University of Miami, Miami, FL 33149, USA

Abstract

A theory for water waves created by the impact of small objects such as raindrops on an initially quiescent body of water is established. Capillary and dissipative viscous effects are taken into account in addition to gravity. It is shown that the prevailing waves are in a mixed capillary–gravity regime around a wavenumber km which corresponds to the minimum value of the group velocity. The waves are described as function of time and distance by the linear superposition of two transient wave components, a ‘sub-km’ (k < km) component and a ‘super-km’ (k > km) component. The super-km components prevail at a short distance from the drop, whereas only the sub-km ones remain at a larger distance. The relative time history of the wavetrain is independent of the size of the drop, and its amplitude is proportional to the drop momentum when it hits the free surface. The wave pattern is composed of a multiplicity of rings of amplitude increasing towards the drop location and is terminated by a trailing wave with an exponential decay. The number of rings increases with time and distance.

Type
Research Article
Copyright
© 1988 Cambridge University Press

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References

Abramovitz, M. & Stegun, I. A.1965 Handbook of Mathematical Functions. Dover Press.
Crapper, G. D.1984 Introduction to Water Waves. Wiley Press.
Dorrestein, R.1951 General linearized theory of the effect of surface films on water ripple. Ken. Ned. Akad. Wet. B. 54, 260272.Google Scholar
Gunn, R. & Kinzer, G. D.1949 The terminal velocity of fall of water droplets in stagnant air. J. Met. 6, 243248.Google Scholar
Horton, R. E.1948 Statistical distribution of drop sizes and the occurrence of dominant drop sizes in rain. Trans. Am. Geophys. Un. 29, 624630.Google Scholar
Jeffreys, H. & Jeffreys, B. S.1956 Methods of Mathematical Physics. Cambridge University Press.
Kajiura, K.1963 The leading wave of a tsunami. Bull. Earthquake Res. Inst. 41, 535571.Google Scholar
Kranzer, H. C. & Keller, J. B.1950 Water waves produced by explosion. J. Appl. Phys. 30, 398407.Google Scholar
Lamb, H.1932 Hydrodynamics. Cambridge University Press.
Le MÉHautÉ, B. 1970 Explosion generated water waves. 8th Symp. on Naval Hydrodynamics, pp. 7191. ONR.
Le MÉHautÉ, B., Wang, S. & Lu, C. C. 1987 Spikes, domes and cavities. J. Intl. Assoc. Hydraul. Res. 5, 583602.Google Scholar
Lhermitte, R. M.1971 Probing of atmospheric motion by airborne pulse-doppler radar techniques. J. Appl. Met. 10, 234246.Google Scholar
Phillips, O. M.1966 The Dynamics of the Upper Ocean. Cambridge University Press.
Van Dorn, W. G. 1966 Boundary dissipation of oscillatory waves. J. Fluid Mech. 24, 769779 and Corrigenda 32 (1968), 828–829.Google Scholar
Whitham, G. B.1974 Linear and Nonlinear Waves. Wiley-Interscience Press.