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The elastodynamics of moving loads, Part 1: The field of a semi-infinite line load moving on the surface of an elastic solid with constant supersonic velocity

Published online by Cambridge University Press:  09 April 2009

Michael Papadopoulos
Affiliation:
Mathematica Research CentreUnited States Army, University of Wisconsin, and Univeristy of Melbourne.
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Abstract

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When a semi-infinite line load moves lengthways, at supersonic velocity, on the plane surface of an elastic solid, the resulting velocity field is conical. There are two characteristic cones, one associated with dilatation effects and the other with shear effects. The propagation process is more complicated than the well-known case of conical flow in supersonic aerodynamics not only because of the presence of two cones of discontinuity but also because the presence of a free surface implies interaction between shear and dilatation effects. It is the interaction process at the free surface which is examined in detail in this paper.

The results of this fundamental problem may be extended by the process of superposition to more general steadily moving loads. In particular by differentiating with respect to time, the potential of a steadily moving point load is obtained explicitly.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 1963

References

[1]Payton, R. G., (Private Communication).Google Scholar
[2]Lamb, H. (1904) On the propagation of tremors over the surface of an elastic solid, Trans. Roy. Soc. A. 203, 142.Google Scholar
[3]Cagniard, L. (1939) Refexion et refraction des ondes seismiques progressives. Paris: Gauthier-Villars.Google Scholar
[4]Lapwood, E. R. (1949), The disturbances due to a line source in a semi-infinite eiastic medium. Phil. Trans. Roy. Soc. A 242, 63100.Google Scholar
[5]Pekeris, C. L. (1955), The seismic surface pulse. Proc. Nat. Acad. Sd. Wash. 41, 469480.CrossRefGoogle ScholarPubMed
[6]Strick, E. (1959), Propagation of elastic wave motion from an impulsive source along a fluid/solid interface. Phil. Trans. Roy. Soc. A. 251, 465533.Google Scholar
[7]Craggs, J. W. (1960) Two dimentional waves in an elastic half-space. Proc. Camb. Phil. Soc. 56 269.CrossRefGoogle Scholar
[8]Maue, A. W. (1954), Die Enstpannungswelle bei-plötzlichen Einschnitt eines gespannten Elastischen Korpers. Zeit. f. Ang. Math. und Mech. 34, 112.CrossRefGoogle Scholar
[9]Miles, J. W. (1960), Homogeneous solutions in elastic wave propagation. Quart. App. Math. 18, 3759.CrossRefGoogle Scholar
[10]Papadopoulos, V. M. (1960), A line source on the interface between a fluid and an elastic solid. Proc. Roy. Soc. A 257, 515533.Google Scholar
[11]Ward, G. N. and Goldstein, S. (1950), The linearized theory of conical fields in supersonic flow, with applications to plane aerofoils. Aero. Quart. 2, 39.Google Scholar
[12]Sternberg, E. (1960) On the integration of the equations of motion in the classical theory of elasticity. Archive Rat. Mech. and Anal. 6, 3450.CrossRefGoogle Scholar
[13]Rayleigh, Lord (1888) On point-, line- and plane-sources of sound. Prc. Lond. Math. Soc. 19, 504507.Google Scholar