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Journal ArticleDOI

The impulse response of a Maxwell Earth

W. R. Peltier
- 01 Nov 1974 - 
- Vol. 12, Iss: 4, pp 649-669
TLDR
In this paper, an extended form of the correspondence principle is employed to determine directly the quasi-static deformation of viscoelastic earth models by mass loads applied to the surface.
Abstract
An extended form of the correspondence principle is employed to determine directly the quasi-static deformation of viscoelastic earth models by mass loads applied to the surface. The stress-strain relation employed is that appropriate to a Maxwell medium. Most emphasis is placed on the discussion of spherically stratified self-gravitating earth models, although some consideration is given to the uniform elastic half space and to the uniform viscous sphere, since they determine certain limiting behaviors that are useful for interpretation and proper normalization of the general problem. Laplace transform domain solutions are obtained in the form of ‘s spectra’ of a set of viscoelastic Love numbers. These Love numbers are defined in analogy with the equivalent elastic problem. An efficient technique is described for the inversion of these s spectra, and this technique is employed to produce sets of time dependent Love numbers for a series of illustrative earth models. These sets of time dependent Love numbers are combined to produce Green functions for the surface mass load boundary value problem. Through these impulse response functions, which are obtained for radial displacement, gravity anomaly, and tilt, a brief discussion is given of the approach to isostatic equilibrium. The response of the earth to an arbitrary quasi-static surface loading may be determined by evaluating a space-time convolution integral over the loaded region using these response functions.

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Citations
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Journal ArticleDOI

The equilibrium form of a rotating earth with an elastic shell

TL;DR: In this article, the authors compute the perturbation to the Earth's equilibrium form due to the presence of a thin elastic lithospheric shell using viscoelastic Love number theory.
Journal ArticleDOI

Vertical deformation and absolute gravity

TL;DR: In this article, the relationship between the displacement field and the gravitational disturbance for a viscoelastic Maxwell Earth with an arbitrary radial viscosity profile was explored, and it was shown that the non-elastic effects of viscous relaxation in the memory of surface mass change can be separated from the effects of present day mass variation by combined measurements of vertical displacement and absolute gravity.
Journal ArticleDOI

Very High-Density Planets: A Possible Remnant of Gas Giants

TL;DR: This study shows that for moderate viscosity values (1025 Pa s or lower), large values of escape rate and associated unloading stress rate during the atmospheric loss process lead to the explosion of extremely massive planets, but for moderate escape rate, the bulk viscosities and finite-strain incompressibility of the cores of giant planets can be large enough to retain a very high density during geological time scales.
References
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Journal ArticleDOI

Diffusional Viscosity of a Polycrystalline Solid

TL;DR: In this article, it is suggested that mosaic boundaries and boundaries between grains of nearly the same orientation may not serve as sources or sinks of the diffusion currents, in which case the creep rate will depend only on the configuration of grain boundaries having a sizable orientation differen...
Journal ArticleDOI

Deformation of the Earth by surface loads

TL;DR: In this article, the static deformation of an elastic half-space by surface pressure is reviewed and a brief mention is made of methods for solving the problem when the medium is plane-strategized, but the major emphasis is on the solution for spherical, radially stratified, gravitating earth models.
Journal ArticleDOI

The Resolving Power of Gross Earth Data

TL;DR: In this article, the authors show how to determine whether a given finite set of gross Earth data can be used to specify an Earth structure uniquely except for fine-scale detail, and the shortest length scale which the given data can resolve at any particular depth.
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