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3D geometry of the strain‐field at transform plate boundaries: Implications for seismic rupture
Author(s) -
Bodin P.,
Bilham R.
Publication year - 1994
Publication title -
geophysical research letters
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.007
H-Index - 273
eISSN - 1944-8007
pISSN - 0094-8276
DOI - 10.1029/94gl02279
Subject(s) - geology , seismology , slip (aerodynamics) , shear zone , seismic moment , shear (geology) , geometry , crust , shear stress , stress field , fault (geology) , geophysics , mechanics , petrology , finite element method , physics , tectonics , mathematics , thermodynamics
We examine the amplitude and distribution of slip on vertical frictionless faults in the zone of concentrated shear strain that is characteristic of transform plate boundaries. We study both a 2D and a 3D approximation to this strain field. Mean displacements on ruptures within the zone of concentrated shear strain are proportional to the shear strain at failure when they are short, and are limited by plate displacements since the last major earthquake when they are long. The transition between these two behaviors occurs when the length of the dislocation approaches twice the thickness of the seismogenic crust, approximately the breadth of the zone of concentrated shear strain observed geodetic ally at transform plate boundaries. This result explains the observed non‐linear scaling relation between seismic moment and rupture length. A geometrical consequence of the 3D model, in which the strain‐field tapers downward, is that moderate earthquakes with rupture lengths similar to the thickness of the crust tend to slip more at depth than near the surface. Seismic moments estimated from surface slip in moderate earthquakes (M≤7) will thus be underestimated. Shallow creep, if its along‐strike dimension is extensive, can reduce a surface slip deficit that would otherwise develop on faults on which M<7 events are typical. In the absence of surface creep or other forms of off‐fault deformation great earthquakes may be necessary features of transform boundaries with downward‐tapering strain‐fields.