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Magnetic and clast fabrics as measurements of grain‐scale processes within the Death Valley shallow crustal detachment faults
Author(s) -
Hayman Nicholas W.,
Housen B. A.,
Cladouhos T. T.,
Livi K.
Publication year - 2004
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 - 10.1029/2003jb002902
Subject(s) - geology , breccia , fault gouge , slip (aerodynamics) , fault (geology) , clastic rock , anisotropy , petrology , mineralogy , seismology , geochemistry , sedimentary rock , physics , thermodynamics , quantum mechanics
The rock product of shallow‐crustal faulting includes fine‐grained breccia and clay‐rich gouge. Many gouges and breccias have a fabric produced by distributed deformation. The orientation of fabric elements provides constraints on the kinematics of fault slip and is the structural record of intrafault strain not accommodated by planar and penetrative surfaces. However, it can be difficult to quantify the deformational fabric of fault rocks, especially the preferred orientations of fine‐grained minerals, or to uniquely determine the relationship between fabric geometry and finite strain. Here, we present the results of a fabric study of gouge and breccia sampled from low‐angle normal (detachment) faults in the Black Mountains, Death Valley, CA. We measured a preferred orientation of the long axes of the clasts inherited from the crystalline footwall of the fault and compared the shape preferred orientation to the anisotropy of magnetic susceptibility of the fault rocks. The two measurements of fabric exhibit systematic similarities and differences in orientation and anisotropy that are compatible with the large‐scale kinematics of fault slip. The dominant carriers of the magnetic susceptibility are micron‐ and sub‐micron scale iron oxides and clay minerals. Therefore even the finest grains in the fault rock were sensitive to the distributed deformation and the micro‐mechanics of particle interaction must have departed from those assumed by the passive‐marker kinematic model that best explains the fabric.

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