Postseismic relaxation theory on the spherical earth

Abstract Postseismic displacements and strains observed at the earth9s surface can be explained through the relaxation of a viscoelastic asthenosphere underlying a purely elastic crust. A theory is presented for modeling the effects of postseismic relaxation on a spherically symmetric earth. For an earthquake point source located in the upper elastic layer, the displacement field is decomposed into its toroidal and spheroidal components. A linear (Maxwell) rheology in the viscoelastic layers is assumed, enabling the use of the correspondence principle for the solutions of the equations of static equilibrium. Displacement and strain fields are then calculated using normal mode summation. Computational results are presented for two simple earthquake sources: a strike slip fault and a uniaxial thrust fault. The patterns of postseismic displacements and strains are found to depend strongly on both the earth model and earthquake source geometry. In particular, the elastic plate thickness, asthenosphere thickness, fault type, and fault length each play a major role in determining the spatial pattern of postseismic relaxation effects. Asthenospheric viscosity controls the temporal pattern of relaxation.

[1]  F. Gilbert,et al.  An application of normal mode theory to the retrieval of structural parameters and source mechanisms from seismic spectra , 1975, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[2]  I. Sacks,et al.  Asthenospheric viscosity inferred from correlated land–sea earthquakes in north-east Japan , 1988, Nature.

[3]  D. Jackson,et al.  A three-dimensional viscoelastic model of a strike slip fault , 1977 .

[4]  J. Rundle,et al.  A viscoelastic coupling model for the cyclic deformation due to periodically repeated Earthquakes at subduction zones , 1984 .

[5]  I. Sacks,et al.  Asthenospheric Viscosity and Stress Diffusion: A Mechanism to Explain Correlated Earthquakes and Surface Deformations In Ne Japan , 1990 .

[6]  J. Rundle An approach to modeling present‐day deformation in southern California , 1986 .

[7]  P. Molnar,et al.  FAULTING ASSOCIATED WITH LARGE EARTHQUAKES AND THE AVERAGE , 1984 .

[8]  J. Rice,et al.  Stress diffusion along rupturing plate boundaries , 1981 .

[9]  A. R. Edmonds Angular Momentum in Quantum Mechanics , 1957 .

[10]  Quasi-static displacements due to faulting in a layered half-space with an intervenient viscoelastic layer. , 1981 .

[11]  H. Melosh Vertical movements following a dip‐slip earthquake , 1983 .

[12]  T. Tabei CRUSTAL MOVEMENTS IN THE INNER ZONE OF SOUTHWEST JAPAN ASSOCIATED WITH STRESS RELAXATION AFTER MAJOR EARTHQUAKES , 1989 .

[13]  J. C. Savage,et al.  Strain accumulation in southern California, 1973–1984 , 1986 .

[14]  Steven C. Cohen Postseismic deformation due to subcrustal viscoelastic relaxation following dip-slip earthquakes , 1984 .

[15]  M. Toksöz,et al.  Time‐dependent deformation and stress relaxation after strike slip earthquakes , 1981 .

[16]  W. Peltier,et al.  Viscous gravitational relaxation , 1982 .

[17]  P. Silver,et al.  Elevation changes and the Great 1960 Chilean Earthquake: Support for aseismic slip , 1989 .

[18]  J. C. Savage,et al.  Asthenosphere readjustment and the earthquake cycle , 1978 .

[19]  F. Wyatt Measurements of coseismic deformation in southern California: 1972–1982 , 1988 .

[20]  D. Turcotte,et al.  Comment on 'An Analysis of Strain Accumulation on a Strike Slip Fault' , 1974 .

[21]  John B. Rundle,et al.  Viscoelastic‐gravitational deformation by a rectangular thrust fault in a layered Earth , 1982 .

[22]  M. Kramer,et al.  Crustal deformation, the earthquake cycle, and models of viscoelastic flow in the asthenosphere , 1984 .

[23]  J. G. Rosenbaum Theory of warping of southern Alaska before Alaska Earthquake, 1964 , 1974 .

[24]  K. Suyehiro,et al.  Episodic aseismic earthquake precursors , 1988, Nature.

[25]  T. Iwasaki Quasi-static deformation due to a dislocation source in a Maxwellian viscoelastic earth model. , 1985 .

[26]  G. Tselentis,et al.  Stress transfer and nonlinear stress accumulation at the North Anatolian fault, Turkey , 1990 .

[27]  V. Li,et al.  Stress transfer and nonlinear stress accumulation at subduction-type plate boundaries — Application to the Aleutians , 1984 .

[28]  J. Rice,et al.  Preseismic rupture progression and great earthquake instabilities at plate boundaries , 1983 .

[29]  S. Ward Quasi-static propagator matrices: Creep on strike-slip faults , 1985 .

[30]  J. C. Savage STRAIN ACCUMULATION IN WESTERN UNITED STATES , 1983 .

[31]  F. Dahlen The spectra of unresolved split normal mode multiplets , 1979 .

[32]  J. Rundle Viscoelastic crustal deformation by finite quasi‐static sources , 1978 .

[33]  Quasi-static Motions near the San Andreas Fault Zone , 1958 .