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Tectonic drivers of the Wrangell block: Insights on fore‐arc sliver processes from 3‐D geodynamic models of Alaska
Author(s) -
Haynie K. L.,
Jadamec M. A.
Publication year - 2017
Publication title -
tectonics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.465
H-Index - 134
eISSN - 1944-9194
pISSN - 0278-7407
DOI - 10.1002/2016tc004410
Subject(s) - geology , subduction , seismology , slab , sinistral and dextral , oblique case , fault (geology) , shear (geology) , strike slip tectonics , slip (aerodynamics) , shear zone , tectonics , transform fault , earthquake rupture , plate tectonics , geophysics , paleontology , linguistics , philosophy , physics , thermodynamics
Intracontinental shear zones can play a key role in understanding how plate convergence is manifested in the upper plate in regions of oblique subduction. However, the relative role of the driving forces from the subducting plate and the resisting force from within intracontinental shear zones is not well understood. Results from high‐resolution, geographically referenced, instantaneous 3‐D geodynamic models of flat slab subduction at the oblique convergent margin of Alaska are presented. These models investigate how viscosity and length of the Denali fault intracontinental shear zone as well as coupling along the plate boundary interface modulate motion of the Wrangell block fore‐arc sliver and slip across the Denali fault. Models with a weak Denali fault (10 17 Pa s) and strong plate coupling (10 21 Pa s) were found to produce the fastest motions of the Wrangell block (∼10 mm/yr). The 3‐D models predict along‐strike variation in motion along the Denali fault, changing from dextral strike‐slip motion in the eastern segment to oblique convergence toward the fault apex. Models further show that the flat slab drives oblique motion of the Wrangell block and contributes to 20% (models with a short fault) and 28% (models with a long fault) of the observed Quaternary slip rates along the Denali fault. The 3‐D models provide insight into the general processes of fore‐arc sliver mechanics and also offer a 3‐D framework for interpreting hazards in regions of flat slab subduction.