Rocky Mountain (66th Annual) and Cordilleran (110th Annual) Joint Meeting (19–21 May 2014)

Paper No. 2
Presentation Time: 1:30 PM

THREE-DIMENSIONAL GEOMETRY OF PSEUDOTACHYLYTE-BEARING FAULTS


RESOR, Phillip G.1, SHERVAIS, Katherine A.H.2, BESSEY, Sarah1, DI TORO, Giulio3 and GRIFFITH, W. Ashley4, (1)Earth and Environmental Sciences, Wesleyan University, 265 Church St, Middletown, CT 06459, (2)Department of Geosciences, Colorado State University, Fort Collins, CO 80523, (3)Dipartimento di Geoscienze, University of Padova, via G. Gradenigo, 6, Padova, 35131, Italy, (4)Earth and Environmental Sciences, University of Texas at Arlington, Geoscience Building Room 107, 500 Yates St. Box 19049, Arlington, TX 76019, presor@wesleyan.edu

Pseudotachylyte is widely considered to be the most reliable indicator of seismogenic slip in ancient fault zones and has thus received significant attention (e.g. Snoke et al., Eds., 1998), even though it appears to be relatively rare. The recent development of high-velocity shear apparatuses has rekindled interest in pseudotachylyte-bearing faults. Dynamic friction experiments in granitoid or gabbroic rocks that achieve earthquake slip velocities reveal significant weakening by melt-lubrication. Extrapolation of these results to seismic source depths (> 7 km) suggests that the slip weakening distance (Dw) over which this transition occurs is < 10 cm. The physics of this lubrication in the presence of a fluid (melt) is controlled by surface micro-topography. In order to characterize fault surface microroughness and its evolution during dynamic slip events on natural faults, we have undertaken an analysis of 3D fault surface microtopography and its causes on a suite of pseudotachylyte-bearing fault strands from the Gole Larghe fault zone, Italy.

The solidification of frictional melt soon after seismic slip ceases “freezes in” earthquake source geometries, however it also precludes the development of extensive fault surface exposures that have enabled direct studies of fault surface roughness. We have overcome this difficulty by imaging the intact 3D geometry of the fault using high-resolution X-ray computed tomography (CT). We collected a suite of 2-3.5 cm diameter cores (2-8 cm long) from individual faults within the Gole Larghe fault zone with a range of orientations (+/- 45 degrees from average strike) and slip magnitudes (0-1 m). Samples were scanned at the University of Texas High Resolution X-ray CT Facility. Individual voxels (3D pixels) are ~36 μm across. Pseudotachylyte-bearing fault zones are imaged as tabular bodies of intermediate X-ray attenuation crosscutting high attenuation biotite and low attenuation quartz and feldspar of the surrounding tonalite. We extract the fault surfaces (contact between Pseudotachylyte and wall rock) to create a digital elevation model for each side of the fault zone and thus quantify melt thickness, volume, and surface microroughness and explore the relationship between these properties and the geometry, slip magnitude, and wall rock mineralogy of the fault.