TY - JOUR
T1 - Stable Forearc Stressed by a Weak Megathrust
T2 - Mechanical and Geodynamic Implications of Stress Changes Caused by the M = 9 Tohoku-Oki Earthquake
AU - Wang, Kelin
AU - Brown, Lonn
AU - Hu, Yan
AU - Yoshida, Keisuke
AU - He, Jiangheng
AU - Sun, Tianhaozhe
N1 - Funding Information:
All the data used in this paper have been previously published in referenced papers. We thank the associate editor and two anonymous reviewers for their comments and M. Sypus for assistance in producing Figure b. L. B. was supported by a Discovery Grant to K. W. from the Natural Sciences and Engineering Research Council of Canada. This is Geological Survey of Canada contribution 20180417.
Funding Information:
All the data used in this paper have been previously published in referenced papers. We thank the associate editor and two anonymous reviewers for their comments and M. Sypus for assistance in producing Figure 2b. L. B. was supported by a Discovery Grant to K. W. from the Natural Sciences and Engineering Research Council of Canada. This is Geological Survey of Canada contribution 20180417.
Publisher Copyright:
© 2019. American Geophysical Union and Her Majesty the Queen in Right of Canada. Reproduced with permission by Natural Resources Canada.
PY - 2019/6
Y1 - 2019/6
N2 - Rupture-zone averaged static stress drop in the 2011 M=9 Tohoku-Oki earthquake was less than 5 MPa, but it caused a stress reversal in most of the offshore forearc, although the reversal is less well constrained far offshore by earthquake mechanisms because of 20- to 30-km errors in event depths. Using a finite element model of force balance, we demonstrate that the stress reversal unambiguously indicates (1) a very weak subduction megathrust and (2) very low differential stresses in the forearc. Prior to the reversal, the upper limit of megathrust strength could not be determined from forearc stresses. In the forearc, effects of megathrust friction and gravity are in a fragile balance, and stresses fluctuate around a neutral state in earthquake cycles. If most of the offshore forearc is to be compressive before but extensional after the earthquake, the effective friction coefficient of the megathrust must be ~0.032. Under low differential stresses associated with megathrust weakness, the forearc is generally well below yielding. Applying the concepts of dynamic Coulomb wedge, we show that the inner wedge, and by inference farther landward, stays stable throughout earthquake cycles. The outer wedge is stable most of the time but may occasionally enter a critical state during great earthquakes; its geometry suggests that complete stress drop of the underlying shallow megathrust is unlikely to have happened. We reason that the occurrence of earthquakes and active faulting under low stress in the stable forearc is due to heterogeneities in structure, stress, and/or pore fluid pressure.
AB - Rupture-zone averaged static stress drop in the 2011 M=9 Tohoku-Oki earthquake was less than 5 MPa, but it caused a stress reversal in most of the offshore forearc, although the reversal is less well constrained far offshore by earthquake mechanisms because of 20- to 30-km errors in event depths. Using a finite element model of force balance, we demonstrate that the stress reversal unambiguously indicates (1) a very weak subduction megathrust and (2) very low differential stresses in the forearc. Prior to the reversal, the upper limit of megathrust strength could not be determined from forearc stresses. In the forearc, effects of megathrust friction and gravity are in a fragile balance, and stresses fluctuate around a neutral state in earthquake cycles. If most of the offshore forearc is to be compressive before but extensional after the earthquake, the effective friction coefficient of the megathrust must be ~0.032. Under low differential stresses associated with megathrust weakness, the forearc is generally well below yielding. Applying the concepts of dynamic Coulomb wedge, we show that the inner wedge, and by inference farther landward, stays stable throughout earthquake cycles. The outer wedge is stable most of the time but may occasionally enter a critical state during great earthquakes; its geometry suggests that complete stress drop of the underlying shallow megathrust is unlikely to have happened. We reason that the occurrence of earthquakes and active faulting under low stress in the stable forearc is due to heterogeneities in structure, stress, and/or pore fluid pressure.
KW - 2011 Tohoku-Oki earthquake
KW - dynamic Coulomb wedge
KW - stable forearc
KW - strength of subduction fault
KW - stress change in earthquake cycles
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U2 - 10.1029/2018JB017043
DO - 10.1029/2018JB017043
M3 - Article
AN - SCOPUS:85068236966
SN - 2169-9313
VL - 124
SP - 6179
EP - 6194
JO - Journal of Geophysical Research: Solid Earth
JF - Journal of Geophysical Research: Solid Earth
IS - 6
ER -