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Chapter 7 - Axial Impact on Slender Deformable Bodies

Published online by Cambridge University Press:  08 January 2010

W. J. Stronge
Affiliation:
University of Cambridge
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Summary

Alice laughed. ‘There's no use trying,’ she said, ‘one can't believe impossible things.’ ‘I daresay you haven't had much practice,’ said the Queen. ‘When I was your age, I always did it for half-an-hour a day. Why, sometimes I've believed as many as six impossible things before breakfast.’

Lewis Carroll, Through the Looking Glass (1872)

Axial impact on a deformable body results in a disturbance which initially propagates away from the impact site at a specific speed. This disturbance is a pulse or wave of particle displacement (and consequent stress). Wave propagation relates to propagation of a coherent pulse of stress and particle displacement through a medium at a finite speed. Familiar manifestations of this phenomenon are the transmission of sound through air, water waves across the surface of the sea and seismic tremors through the earth; thus, waves exist in gases, liquids and solids. Sources of excitation may be either concentrated or distributed spatially, and brief or extended functions of time. The unifying characteristic of waves is propagation of a disturbance through a medium. Properties of the medium that result in waves and determine the speeds of propagation are the density ρ and moduli of deformability (Young's modulus E, shear modulus G, bulk modulus K, etc.).

Longitudinal Wave in Uniform Elastic Bar

Consider a uniform slender elastic bar of cross-sectional are A, elastic modulus E and density ρ; the bar contains a region with axial stress σ(x, t) that is propagating in the positive x direction as shown in Fig. 7.1.

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Impact Mechanics , pp. 146 - 172
Publisher: Cambridge University Press
Print publication year: 2000

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