Direct constraints on in situ stress state from deep drilling into the Nankai subduction zone, Japan

Author:

Tobin Harold J.1,Saffer Demian M.2,Castillo David A.3,Hirose Takehiro4

Affiliation:

1. 1Department of Earth and Space Sciences, University of Washington, Box 351310, Seattle, Washington 98195, USA

2. 2Institute for Geophysics and Department of Geological Sciences, University of Texas at Austin, 10601 Exploration Way, Austin, Texas 78758, USA

3. 3Insight Geomechanics, 8 Joffre Road, Trigg, Western Australia 6029, Australia

4. 4Kochi Institute for Core Sample Research (X-star), Japan Agency for Marine-Earth Science and Technology, 200 Monobe-otsu Nankoku, Kochi 783-8502, Japan

Abstract

Abstract Stress state is a long-sought but poorly known parameter on subduction megathrusts and in overlying accretionary wedges in general. We used direct observations made during drilling of Integrated Ocean Drilling Program (IODP) borehole C0002 to a depth of 3058 m below the seafloor (mbsf) in the Nankai subduction zone of southwestern Japan to constrain in situ pore pressure and stress state in the deep interior of an accretionary wedge for the first time. These data included downhole pressure, active pumping tests, and logging and sample measurements. We found a nearly linear gradient in minimum horizontal principal stress (Shmin) and show that it remained consistently smaller than the vertical stress (Sv), definitively ruling out a thrust-faulting stress regime to at least 3 km depth, and to within ~2 km above the subduction megathrust. At 3000 mbsf, the estimated effective stresses were: Sv = 33 MPa, SHmax = 25–36 MPa, and Shmin = 18.5–21 MPa. We therefore interpret that the stress state throughout the drilled interval, which lies entirely in the hanging wall of the active megathrust, lies in a normal or strike-slip faulting regime (Sv ≥ SHmax > Shmin). Total differential stresses are below ~18 MPa. We conclude that (1) basal traction along the megathrust must be small in order to permit both locking (and frictional sliding at failure) of the décollement and such low differential stresses deep within the upper plate; and (2) although differential stresses may remain low all the way to the plate boundary at ~5000 mbsf, SHmax must transition to become greater than the vertical stress—either spatially below the base of the borehole or temporally leading up to megathrust fault rupture—in order to drive thrust motion along the plate boundary as observed in great earthquakes and in recurring very low-frequency earthquakes and slow-slip events.

Publisher

Geological Society of America

Subject

Geology

Reference32 articles.

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