DUCTILE CREEP AND COMPACTION - A MECHANISM FOR TRANSIENTLY INCREASINGFLUID PRESSURE IN MOSTLY SEALED FAULT ZONES

Citation
Nh. Sleep et Ml. Blanpied, DUCTILE CREEP AND COMPACTION - A MECHANISM FOR TRANSIENTLY INCREASINGFLUID PRESSURE IN MOSTLY SEALED FAULT ZONES, Pure and Applied Geophysics, 143(1-3), 1994, pp. 9-40
Citations number
NO
Categorie Soggetti
Geosciences, Interdisciplinary
Journal title
ISSN journal
00334553
Volume
143
Issue
1-3
Year of publication
1994
Pages
9 - 40
Database
ISI
SICI code
0033-4553(1994)143:1-3<9:DCAC-A>2.0.ZU;2-E
Abstract
A simple cyclic process is proposed to explain why major strike-slip f ault zones, including the San Andreas, are weak. Field and laboratory studies suggest that the fluid within fault zones is often mostly seal ed from that in the surrounding country rock. Ductile creep driven by the difference between fluid pressure and lithostatic pressure within a fault zone leads to compaction that increases fluid pressure. The in creased fluid pressure allows frictional failure in earthquakes at she ar tractions far below those required when fluid pressure is hydrostat ic. The frictional slip associated with earthquakes creates porosity i n the fault zone. The cycle adjusts so that no net porosity is created (if the fault zone remains constant width). The fluid pressure within the fault zone reaches long-term dynamic equilibrium with the (hydros tatic) pressure in the country rock. One-dimensional models of this pr ocess lead to repeatable and predictable earthquake cycles. However, e ven modest complexity, such as two parallel fault splays with differen t pressure histories, will lead to complicated earthquake cycles. Two- dimensional calculations allowed computation of stress and fluid press ure as a function of depth but had complicated behavior with the unacc eptable feature that numerical nodes failed one at a time rather than in large earthquakes. A possible way to remove this unphysical feature from the models would be to include a failure law in which the coeffi cient of friction increases at first with frictional slip, stabilizing the fault, and then decreases with further slip, destabilizing it.