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Creep in the Earth and Planets (Invited Lecture)

Published online by Cambridge University Press:  27 June 2016

Harold Jeffreys*
Affiliation:
St. John's College, Cambridge, England

Abstract

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An outstanding problem is to reconcile the Moon's rotation with the persistence of its non-hydrostatic dynamical ellipticities. The first requires imperfection of elasticity under strains of order 10−7; the second apparently little under larger ones.

Lomnitz gave experimental evidence that creep is linear at elastic shears from 10−5 to 10−4, indicating that a linear rule could be right at still smaller values. Positive evidence for the Earth comes from the damping of the 14-monthly nutation, which has a relaxation time of the order of 30 yr. Most work on imperfect elasticity has assumed that under constant shear stress the strain increases with time either like t (elasticoviscosity) or like logt. If the result from the 14-monthly nutation, with elasticoviscosity, is applied to the Moon, the dynamical ellipticities would have subsided considerably in the last 200 yr. With the logarithmic rule an S pulse at 80° would have its beginning spread out over about 70 s and be unreadable. These contradictions are avoided if the increase under constant stress is about like t0.2. The resulting law involves two constants. Without change of these, applications are made to other phenomena. The rotations of the Moon and of other satellites whose rotations are known are explained; so is the persistence of the Moon's dynamical ellipticities; also the failure to detect three free oscillations that might theoretically exist. Elasticoviscosity would imply rapid disappearance of the non-hydrostatic second and third harmonics in the Earth's gravitational field; this is avoided with the new law. Study of damping of free vibrations of the Earth (including surface waves) has usually assumed the logarithmic law, but it appears that the new law fits the data at least as well, and that it may also explain those that have been interpreted in favour of layers of low velocity. It appears that the damping at depths up to 400 km or so is much more severe than the average for the Earth's shell, and more evidence for shorter periods is much needed.

Any law with an index less than 1 would forbid thermal instability (convection) and continental drift.

Type
Research Article
Copyright
Copyright © Reidel 1972 

References

Alsop, E. E., Sutton, G. H., and Ewing, M.: 1961, J. Geophys. Res. 66, 631.Google Scholar
Alsop, E. E., Sutton, G. H., and Ewing, M.: 1961, J. Geophys. Res. 66, 2911.CrossRefGoogle Scholar
Anderson, D. L. and Archambeau, C. B.: 1964, J. Geophys. Res. 69, 2071.Google Scholar
Anderson, D. L., Ben-Menahem, A., and Archambeau, C. B.: 1965, J. Geophys. Res. 70, 1441.CrossRefGoogle Scholar
Ben-Menahem, A.: 1965, J. Geophys. Res. 70, 4641.Google Scholar
Buchbinder, G. G. R.: 1965, Bull. Seism. Soc. Am. 55, 441.Google Scholar
Bullen, K. E. and Haddon, R. A. W.: 1967, Nature 213, 574.Google Scholar
Derr, J. S.: 1969, Bull. Seism. Soc. Am. 74, 5202.Google Scholar
Jeffreys, H.: 1956, Quart. J. Mech. Appl. Math. 9, 1.CrossRefGoogle Scholar
Jeffreys, H.: 1958, Geophys. J. Roy. Astron. Soc. 1, 162.Google Scholar
Jeffreys, H.: 1965, Nature 208, 675.Google Scholar
Jeffreys, H. and Jeffreys, B. S.: 1966, Methods of Mathematical Physics, Camb. Univ. Press.Google Scholar
Jeffreys, H. and Vicente, R. O.: 1967, Acad. Roy. Belg. Bull. Cl. Sci. (5) 53, 926.Google Scholar
Jeffreys, H.: 1970, The Earth, esp. pp. 1213, 47, 331–334, 490, 494.Google Scholar
Jeffreys, H. and Crampin, S.: 1970, Monthly Notices Roy. Astron. Soc. 147, 295.CrossRefGoogle Scholar
Landisman, M., Sato, Y., and Nafe, J.: 1965, Geophys. J. Roy. Astron. Soc. 9, 439.Google Scholar
Wiggins, M. A.: 1968, Phys. Earth Planetary Int. 1, 201.Google Scholar