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Dynamic elastic moduli of a suspension of imperfectly bonded spheres

Published online by Cambridge University Press:  24 October 2008

A. K. Mal
Affiliation:
Mechanics and Structures Department, University of California, Los Angeles
S. K. Bose
Affiliation:
Mechanics and Structures Department, University of California, Los Angeles

Abstract

An isotropic elastic material containing a random distribution of identical spherical particles of another elastic material is considered. The bonding between the spheres and the matrix is imperfect, so that slip may occur at interfaces when stress is applied to the medium. The shear stresses at the interface is assumed to be proportional to the amount of slip. The velocity and attenuation of the average harmonic elastic waves propagating through such a medium are calculated. The results are valid to the lowest order in frequency for wave lengths long compared with the radius of the sphere. The dynamic elastic moduli are obtained from these results and are compared with available results for welded contact. The variations in the P and S wave velocities for propagation across earthquake faults is discussed.

Type
Research Article
Copyright
Copyright © Cambridge Philosophical Society 1974

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References

REFERENCES

(1)Mal, A. K. and Knopoff, L.Elastic wave velocities in two component systems. J. Inst. Math. Appl. 3 (1967), 376387.CrossRefGoogle Scholar
(2)Barratt, P. J.Multiple scattering of plane harmonic elastic waves in an infinite solid by an arbitrary configuration of obstacles. Proc. Cambridge. Philos. Soc. 66 (1969), 469480.CrossRefGoogle Scholar
(3)Lax, M.Multiple scattering of waves, II. Phys. Rev. 85 (1952), 621629.CrossRefGoogle Scholar
(4)Fikioris, J. G. and Waterman, P. C.Multiple scattering of waves, II - Hole corrections in scalar case. J. Math. Phys. 5 (1964), 14131420.CrossRefGoogle Scholar
(5)Stratton, J. A.Electromagnetic theory (McGraw-Hill; New York, 1941), 414419.Google Scholar
(6)Batchelor, G. K. and Green, J. T.The determination of the bulk stress in a suspension of spherical particles to order c 2. J. Fluid Mech. 56 (1972), 401427.CrossRefGoogle Scholar
(7)Morse, P. M. and Feshbach, H.Methods of theoretical physics, part II (McGraw-Hill; New York, 1953), 1899.Google Scholar
(8)Walpole, L. J.The elastic behaviour of a suspension of spherical particles. Quart. J. Mech. Appl. Math. 25 (1972), 153160.CrossRefGoogle Scholar
(9)Kerner, E. H.The elastic and thermoelastic properties of composite media. Proc. Phys. Soc. (B) 69 (1956), 808813.CrossRefGoogle Scholar
(10)Nur, A.Dilatancy, pore fluids and premonitory variations of tp/ts travel times. Bull Seism. Soc. Am. 62 (1972), 12171222.CrossRefGoogle Scholar
(11)Cruzan, O. R.Translational addition theorems for spherical vector wave equations. Quart. Appl. Math. 20 (1962), 3340.CrossRefGoogle Scholar