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Effects of the extrusion of fault gouge on frictional sliding
Author(s) -
Sleep Norman H.
Publication year - 1999
Publication title -
journal of geophysical research: solid earth
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.67
H-Index - 298
eISSN - 2156-2202
pISSN - 0148-0227
DOI - 10.1029/1999jb900240
Subject(s) - fault gouge , traction (geology) , shear (geology) , geology , dilatant , slip (aerodynamics) , extrusion , geotechnical engineering , strain rate , mechanics , imbrication , materials science , fault (geology) , composite material , physics , thermodynamics , petrology , seismology , tectonics , geomorphology
Thick gouge is extruded from between sample contacts of simulated fault zones. Thin gouge is locally extruded by irregularities of the fault surfaces. Extrusion causes the simple shear strain rate ε ˙ to vary as a function of position within the gouge and with time. The local shear traction thus varies from its macroscopic value. The case of thick gouge is quantitatively modeled. Extrusion does not significantly affect experiments measuring a and b in the traditional formula for the instantaneous coefficient of friction μ = μ 0 + a ln ( ε ˙ / ε ˙ 0 ) + b ln ( Ψ ) , where μ 0 is the steady state coefficient of friction at the reference strain rateε ˙ 0and the state variable ψ depends on the previous history of the sample. Other effects are modest and most likely to be observable when a > b , implying that the strain rate does not spontaneously localize. The macroscopic coefficient of friction for a > b is decreased by an amount which is less than the short/long aspect ratio of the gouge zone. Measurments of frictional dilatancy in velocity‐stepping experiments and of the effects of sudden changes of normal traction on shear traction are not compromised if the plates bounding the fault gouge behave as rigid parallel planes. The changes in shear traction after a sudden change in normal traction are strongly affected if the walls confining the gouge are compliant and do not remain parallel. Then the local ratio of the new normal traction to the old normal traction varies with position on the fault surface.

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