GSA Connects 2023 Meeting in Pittsburgh, Pennsylvania

Paper No. 253-11
Presentation Time: 4:15 PM

QUANTIFYING PORE-FLUID PRESSURE RATIOS AND ANALYZING DEFORMATION MECHANISMS IN THE WHIPPLE MOUNTAINS BRITTLE-DUCTILE SHEAR ZONE


JARAMILLO, Valeria, Earth, Planetary, and Space Sciences, University of California, Los Angeles, 595 Charles Young Drive East, Los Angeles, CA 90095, YIN, An, Dept of Earth, Planetary, and Space Sciences, University of California, Los Angeles, Los Angeles, CA 90095, CATLOS, E.J., Jackson School of Geosciences, The University of Texas at Austin, 2275 Speedway Stop C9000, Austin, TX 78712, BELL, Elizabeth, Earth, Planetary, and Space Sciences, UCLA, Los Angeles, CA 90095, CHIN, Emily J., Scripps Institution of Oceanography, University of California San Diego, 9500 Gilman Drive, La Jolla, CA 92093 and SCHMITT, Axel K., John de Laeter Centre, Curtin University, Kent St, Bentley, 6102, Australia; Institute of Earth Sciences, Heidelberg University, Ruprecht-Karls-Universität Heidelberg Im Neuenheimer Feld 236, Heidelberg, D-69120, Germany

Pore-fluid pressure is a key factor controlling the stress state and rock failure in Earth’s crust. Although its role in brittle deformation in the shallow crust (< 1-3 km) has been extensively examined, and in some cases quantified by direct bore-hole measurements, how pore-fluid pressure affects crustal deformation at brittle-ductile-transition depths (~15-25 km) remains poorly constrained. Deformation that occurred at brittle-ductile transition depths is commonly expressed by the development of semi-brittle shear zones characterized by coeval cataclastically (frictional sliding and fracturing) and crystal-plastically (dislocation and diffusion creep) of deformed rocks. The distinct deformation styles within the same shear zone require stress continuity across the contact between brittle and ductile structures. This stress-continuity condition in turn allows us to use paleobarometry and paleopiezometry to determine the stress state (i.e., the differential stress and mean stress) during semi-brittle deformation. Because the frictional coefficient (~0.6) and cohesive strength of crystalline rocks (<50 MPa) are well-known from laboratory experiments (i.e. Byerlee’s Law), we are able to use the estimated differential and mean stresses to determine the ratio between pore-fluid pressure and lithostatic pressure during the development of the Whipple detachment shear zone. Our results suggest pore-fluid pressure ratios between 0.92 and 1.11 which is consistent with observed tensile-fracture veins (pore-fluid pressure ratio >1.0) developed during the crystal-plastic deformation of quartzite in the shear zone. New P-T and monazite-in-garnet U/Th-Pb age constraints combined with the pore-fluid pressure ratios provide insights into the evolution of the Whipple detachment shear zone. A new P-T-t path may be established for the rocks in the Whipple shear zone and may suggest a deeper initiation or multiple metamorphic events not previously analyzed.