Reassessment of the Maximum Fault Rupture Length of Strike‐Slip Earthquakes and Inference on Mmax in the Anatolian Peninsula, Turkey

Seismic‐hazard analyses and stress tests for critical infrastructures show limitations in the treatment of extreme events. These extreme events can be great earthquakes and/or their cascading effects, generally not foreseen in risk analysis and management (e.g., Komendantova et al. , 2014). For instance, earthquake ruptures are known to potentially propagate over several segments (e.g., Eberhart‐Phillips et al. , 2003; Fliss et al. , 2005), yet fault segments are still modeled as individual faults in most regional seismic‐hazard models based on expert opinion and on limited paleoseismic data. Rate anomalies (known as the bulge) in the Uniform California Earthquake Rupture Forecast, Version 2 (UCERF2) are in part due to the neglect of possible links between fault segments (Field et al. , 2009). Recent catastrophes, such as the 2011 M w 9.0 Tohoku earthquake and its consequences (e.g., Norio et al. , 2011), have demonstrated the need for “a targeted reassessment of the safety margins” of critical infrastructures (European Nuclear Safety Regulators Group [ENSREG], 2011). The present study is designed to address the issue of potentially unforeseen great earthquakes (1) by proposing criteria for earthquake rupture cascading over fault segments based on geometrical and physical considerations and (2) by assessing the maximum magnitude ( M max) of these ruptures spanning hundreds of kilometers. Focus is on strike‐slip mechanisms. Different definitions of M max have been proposed based on the assumption that no earthquake is expected above that threshold, such as the maximum observed magnitude, the deterministic “maximum credible” magnitude (Reiter, 1990), and the statistical “maximum possible” magnitude (Kijko and Singh, 2011). The predictive power of the statistical approach has been recently shown to be rather poor (Zoller et al. , 2013). Furthermore, Holschneider et al. (2014) found it is essentially impossible to infer M max from earthquake catalogs alone. Our method to assess M max is directly related to the …

[1]  D. Sanderson,et al.  The relationship between displacement and length of faults: a review , 2005 .

[2]  Sonia Fliss,et al.  Fault branching and rupture directivity , 2002 .

[3]  Nadejda Komendantova,et al.  Multi-hazard and multi-risk decision-support tools as a part of participatory risk governance: feedback from civil protection stakeholders , 2014 .

[4]  H. Kanamori,et al.  The 2012 Sumatra great earthquake sequence , 2012 .

[5]  A. Kijko,et al.  Statistical tools for maximum possible earthquake magnitude estimation , 2011 .

[6]  Steven M. Day,et al.  The 1999 İzmit, Turkey, Earthquake: A 3D Dynamic Stress Transfer Model of Intraearthquake Triggering , 2002 .

[7]  Steven G. Wesnousky,et al.  Predicting the endpoints of earthquake ruptures , 2006, Nature.

[8]  A. Barka,et al.  Strike‐slip fault geometry in Turkey and its influence on earthquake activity , 1988 .

[9]  Timothy E. Dawson,et al.  Uniform California Earthquake Rupture Forecast, Version 2 (UCERF 2) , 2009 .

[10]  Ian G. Main,et al.  Earthquake Hazard Analysis: Issues and insights , 1992 .

[11]  S. Day,et al.  3D simulations of multi‐segment thrust fault rupture , 1999 .

[12]  Timothy E. Dawson,et al.  The 2002 Denali Fault Earthquake, Alaska: A Large Magnitude, Slip-Partitioned Event , 2003, Science.

[13]  Steven M. Day,et al.  Dynamics of fault interaction: parallel strike‐slip faults , 1993 .

[14]  Roberto Basili,et al.  The European Database of Seismogenic Faults (EDSF) compiled in the framework of the Project SHARE. , 2013 .

[15]  Tatiana Goded,et al.  Selection of Earthquake Scaling Relationships for Seismic‐Hazard Analysis , 2013 .

[16]  Steven G. Wesnousky,et al.  Displacement and Geometrical Characteristics of Earthquake Surface Ruptures: Issues and Implications for Seismic-Hazard Analysis and the Process of Earthquake Rupture , 2008 .

[17]  G. King,et al.  STATIC STRESS CHANGES AND THE TRIGGERING OF EARTHQUAKES , 1994 .

[18]  Steven G. Wesnousky,et al.  Earthquake size as a function of fault slip rate , 1996, Bulletin of the Seismological Society of America.

[19]  J. Rice,et al.  Role of fault branches in earthquake rupture dynamics , 2006 .

[20]  James R. Rice,et al.  Dynamic shear rupture interactions with fault bends and off-axis secondary faulting , 2002 .

[21]  M. Holschneider,et al.  The Maximum Earthquake Magnitude in a Time Horizon: Theory and Case Studies , 2013 .

[22]  Barbara Romanowicz,et al.  On moment‐length scaling of large strike slip earthquakes and the strength of faults , 2002 .

[23]  D. Wells,et al.  New empirical relationships among magnitude, rupture length, rupture width, rupture area, and surface displacement , 1994, Bulletin of the Seismological Society of America.

[24]  Nobuki Kame,et al.  Effects of prestress state and rupture velocity on dynamic fault branching , 2002 .

[25]  Developing Seismogenic Source Models Based on Geologic Fault Data , 2011 .

[26]  N. N. Ambraseys,et al.  Some characteristic features of the Anatolian fault zone , 1970 .

[27]  M. Holschneider,et al.  Can we test for the maximum possible earthquake magnitude , 2014 .

[28]  Steven M. Day,et al.  Dynamic 3D simulations of earthquakes on En Echelon Faults , 1999 .

[29]  Gregory C. Beroza,et al.  Source Scaling Properties from Finite-Fault-Rupture Models , 2000 .

[30]  Young-Seog Kim,et al.  Rupture propagation inferred from damage patterns, slip distribution, and segmentation of the 1957 MW8.1 Gobi‐Altay earthquake rupture along the Bogd fault, Mongolia , 2012 .

[31]  Harsha S. Bhat,et al.  DYNAMIC SLIP TRANSFER FROM THE DENALI TO TOTSCHUNDA FAULTS, ALASKA: TESTING THEORY FOR FAULT BRANCHING , 2004 .

[32]  C. Meletti,et al.  Homogeneous determination of maximum magnitude , 2010 .

[33]  P. Shi,et al.  The 2011 eastern Japan great earthquake disaster: Overview and comments , 2011 .

[34]  A. Rosakis,et al.  Cracks faster than the shear wave speed , 1999, Science.

[35]  Thomas C. Hanks,et al.  A Bilinear Source-Scaling Model for M-log A Observations of Continental Earthquakes , 2002 .

[36]  Domenico Giardini,et al.  Setting the Stage for Harmonized Risk Assessment by Seismic Hazard Harmonization in Europe (SHARE) , 2010 .

[37]  M. Leonard Earthquake Fault Scaling: Self‐Consistent Relating of Rupture Length, Width, Average Displacement, and Moment Release , 2010 .