Download Download

Total Page:16

File Type:pdf, Size:1020Kb

Download Download Research in Geophysics 2016; volume 5:5730 Time dependent seismicity Fuca and North America plates corresponds to the Cascadia subduction zone (CSZ), where Correspondence: Evangelos Christou, Planetary along the western coast the giant M9 earthquake occurred in 1700. Sciences Humboldt Universität zu Berlin, of Canada The present study was motivated by the Jablonskistraße 14, Berlin, Germany. occurrence of the 2012 Haida Gwaii islands Tel.: +49.15258299952. Evangelos V. Christou, George Karakaisis, (formerly the Queen Charlotte islands) earth- E-mail: [email protected] Emmanuel Scordilis quake (M=7.7). This was the first major thrust Key words: Time dependent seismicity; Canada; 1 Department of Geophysics, School of event recorded along the strike-slip QCF. In Haida Gwaii 2012 earthquake. this article we present the results of the appli- Geology, Aristotle University of cation of two time-dependent seismicity mod- Acknowledgements: Evangelos Christou grateful- Thessaloniki, Greece els in an attempt to retrospectively predict the ly acknowledges Dr. G. Papadopoulos (Chair) and 2012 mainshock. Moreover, we apply both mod- the Organizing Committee of the International els searching for future strong earthquakes Workshop Mega Earthquakes and Tsunamis in Subduction Zones for the financial support. Maps along the western coast of Canada. Abstract were made using Generic Mapping Tools GMT 4.5 (Wessel and Smith, 1998). We used data from the Models applied and data National Resources Canada (On-line Bulletin), Decelerating generation of intermediate The first of the two time-dependent seismic- http://earthquakescanada.nrcan.gc.ca/stndon/NE magnitude earthquakes (preshocks) in a nar- ity models is based on the triggering of a main- DB-BNDS/bull-eng.php, Nat. Res. Can., (last row region (seismogenic region) and acceler- shock by its preshocks and is called decelerat- accessed: July 23, 2014). We thank the anony- ating generation of relatively larger such mous reviewer for the helpful comments and sug- ing-accelerating seismic strain (D-AS) model. gestions. earthquakes in a broader region (critical There is reliable evidence that an increase in region) has been proposed as an appropriate the occurrence rate of intermediate-magni- Conference presentation: this work has been pre- model for intermediate-term earthquake pre- tude shocks has been observed in a broad area sented in the International Workshop Mega diction. We examined the seismic activity before strong earthquakes.2-8 Recently, howev- Earthquakes and Tsunamis in Subduction Zones- which preceded the Mw=7.7 (October 28, 2012) er, skepticism has been expressed on the reli- Forecasting Approaches and Implications for thrust event that occurred off the west coast of ability of these observations,9,10 which is dis- Hazard Assessment, held in Rhodes Island, Greece (2014). Haida Gwaii, Canada (formerly the Queen cussed later. Quantification of the accelerating Charlotte islands), by applying the decelerat- pattern of these earthquakes that occur in this Received for publication: 24 November 2014. ing-accelerating seismic strain model. We 11 broad region before a mainshock, showed Revision received: 6 December 2015. found that this mainshock was preceded by a that the cumulative Benioff strain, S(t), can be Accepted for publication: 22 December 2015. pronounced accelerating seismic sequence expressed by the following power law: with the time to the mainshock, as well as by This work is licensed under a Creative Commons an equally easily identifiable decelerating seis- Attribution NonCommercial 4.0 License (CC BY- mic sequence. Both precursory seismic (1) NC 4.0). sequences occurred in different space, time and magnitude windows. The behavior of pre- ©Copyright E.V. Christou et al., 2016 where tc is the origin time of the mainshock Licensee PAGEPress, Italy vious mainshocks that occurred close to the and A, B, m, are parameters calculated by the Research in Geophysics 2016; 5:5730 2012 earthquake was also examined by the available data (with m<1, B<0). The quantity doi:10.4081/rg.2016.5730 time and magnitude predictable regional S(t), which is considered as a measure of the model. preshock seismic deformation at time t, is An attempt was also made to identify such seismic strain patterns, which may also be defined as , where Ei is the (M=6.3-9.0) shallow (h<100 km) mainshocks related to the generation of strong mainshocks worldwide.15 Tests performed on synthetic cat- along the western coast of Canada. seismic energy of the ith preshocks and n(t) is alogues15,16 and retrospective predictions of the number of preshocks occurred up to time t. recent strong mainshocks have been used to On the other hand, it has also been observed evaluate the model whereas forward tests led Non commercialthat in the narrow (focal) region of anuse ensuing only to the successful intermediate-term prediction Introduction mainshock, a seismic excitation is followed by of two strong earthquakes in the Aegean.17,18 a drop of seismicity, i.e., a seismic quiescence During the formulation of the D-AS model it Strong and large earthquakes along the period.12,13 Global data were used14 to show that was observed that each of the investigated western coast of Canada are not uncommon. intermediate magnitude preshocks in the focal During the instrumental period (since 1898, region form a decelerating pattern and that the mainshocks was preceded by a decelerating when the first seismograph of Milne type was time variation of the cumulative Benioff strain preshock sequence, generated in a relatively small region (seismogenic region) where the installed at Victoria) several M≥7.0 events up to the mainshock also follows a power-law occurred there. The majority of the strong (relation 1) but with a power value larger than mainshock is also located, and by an accelerat- earthquakes in this area are associated with one (m>1). That is, this pattern of decelerat- ing preshock sequence generated in a broader the motion between the three major lithos- ing strain in the focal region is formed of a region (critical region) and that both precurso- pheric plates, namely Pacific, North America seismic excitation followed by a decrease of ry seismic sequences have predictive proper- and Juan de Fuca (Figure 1). The boundary seismicity of intermediate magnitude ties, related to the ensuing mainshock. between Pacific and North America plates is a preshocks. Decelerating preshocks occur in different right lateral transform fault (Queen Charlotte The formulation of the D-AS model for inter- time, magnitude and space windows than the Fault, QCF) that extends from Vancouver mediate-term earthquake prediction was accelerating preshocks. The latter start earlier Island up to Alaska and the Fairweather Fault based on the examination of the patterns than the former (tsa>tsd), and their magnitudes (FF), whereas the boundary between Juan de described above, which preceded strong are larger the magnitudes of the decelerating [Research in Geophysics 2016; 5:5730] [page 1] Article preshocks. The strain acceleration, qa, as well parameter and Pd is the probability that a than the relatively short span of the earth- as the strain deceleration, qd, (also called qual- decelerating strain release fulfils relations (2) quake catalogues used, it is preferable to con- ity indexes), vary with the time to the main- and (4). Both quality indexes qd and qa are very sider seismogenic sources, i.e., circular shock.17 Both start with low values, attain their useful in searching for decelerating and accel- regions that include, in addition to the main largest values several years before the main- erating seismicity patterns since they attain fault where the largest mainshock occurs, shock occurrence and cease gradually about their largest values at the seismogenic and other smaller faults where smaller mainshocks three years before the mainshock, i.e., the critical region, respectively. Global observa- occur. On the basis of this idea, the time and seismic activity declines in the critical region tions15 resulted in the following cut-off values magnitude predictable regional (TIMAPR) and increases in the seismogenic region. of the parameters that describe the decelerat- model has been proposed,21 which makes use The radii r (km) of the seismogenic region ing and the accelerating precursory seismic of numerous interevent times of strong earth- and R (km) of the critical region, which are sequences: quakes (mainshocks) generated in a region, in assumed circular, are given by the relations:15 order to investigate the time-dependent seis- (8) micity of this region. This model has been developed by considering a large sample of (9) global data,21 which was used to derive the fol- (2) lowing two equations that relate the interevent The second of the models applied in the time, Tt (in years), until the next mainshock present work makes use of interevent times of and its expected magnitude, Mf, to the magni- (3) strong earthquakes in an area, which depend tude, Mp, of the previous mainshock in the on the rate of tectonic loading. However, since region examined, the long-term seismicity 1/2 such earthquakes, that occur on a single fault, level, Sd (the seismic strain rate in Joule per with M being the mainshock magnitude and sd usually have recurrence times much larger year) and the minimum mainshock magni- 1/2 4 2 and sa (in J /y × 10 km ) is the Benioff strain in the seismogenic and critical region, respec- tively. The following two relations hold also for the decelerating and accelerating preshock sequences:15 (4) (5) where tsd and tsa are the start times (in years) of the decelerating and accelerating preshock sequence, respectively. The curvature parameter, C, has been pro- posed19 as a measure of accelerating strain release and equals to the ratio of the RMS error of the power-law fit (Eq. 1) to the corre- sponding linear fir error.
Recommended publications
  • Coulomb Stresses Imparted by the 25 March
    LETTER Earth Planets Space, 60, 1041–1046, 2008 Coulomb stresses imparted by the 25 March 2007 Mw=6.6 Noto-Hanto, Japan, earthquake explain its ‘butterfly’ distribution of aftershocks and suggest a heightened seismic hazard Shinji Toda Active Fault Research Center, Geological Survey of Japan, National Institute of Advanced Industrial Science and Technology (AIST), site 7, 1-1-1 Higashi Tsukuba, Ibaraki 305-8567, Japan (Received June 26, 2007; Revised November 17, 2007; Accepted November 22, 2007; Online published November 7, 2008) The well-recorded aftershocks and well-determined source model of the Noto Hanto earthquake provide an excellent opportunity to examine earthquake triggering associated with a blind thrust event. The aftershock zone rapidly expanded into a ‘butterfly pattern’ predicted by static Coulomb stress transfer associated with thrust faulting. We found that abundant aftershocks occurred where the static Coulomb stress increased by more than 0.5 bars, while few shocks occurred in the stress shadow calculated to extend northwest and southeast of the Noto Hanto rupture. To explore the three-dimensional distribution of the observed aftershocks and the calculated stress imparted by the mainshock, we further resolved Coulomb stress changes on the nodal planes of all aftershocks for which focal mechanisms are available. About 75% of the possible faults associated with the moderate-sized aftershocks were calculated to have been brought closer to failure by the mainshock, with the correlation best for low apparent fault friction. Our interpretation is that most of the aftershocks struck on the steeply dipping source fault and on a conjugate northwest-dipping reverse fault contiguous with the source fault.
    [Show full text]
  • Intraplate Earthquakes in North China
    5 Intraplate earthquakes in North China mian liu, hui wang, jiyang ye, and cheng jia Abstract North China, or geologically the North China Block (NCB), is one of the most active intracontinental seismic regions in the world. More than 100 large (M > 6) earthquakes have occurred here since 23 BC, including the 1556 Huax- ian earthquake (M 8.3), the deadliest one in human history with a death toll of 830,000, and the 1976 Tangshan earthquake (M 7.8) which killed 250,000 people. The cause of active crustal deformation and earthquakes in North China remains uncertain. The NCB is part of the Archean Sino-Korean craton; ther- mal rejuvenation of the craton during the Mesozoic and early Cenozoic caused widespread extension and volcanism in the eastern part of the NCB. Today, this region is characterized by a thin lithosphere, low seismic velocity in the upper mantle, and a low and flat topography. The western part of the NCB consists of the Ordos Plateau, a relic of the craton with a thick lithosphere and little inter- nal deformation and seismicity, and the surrounding rift zones of concentrated earthquakes. The spatial pattern of the present-day crustal strain rates based on GPS data is comparable to that of the total seismic moment release over the past 2,000 years, but the comparison breaks down when using shorter time windows for seismic moment release. The Chinese catalog shows long-distance roaming of large earthquakes between widespread fault systems, such that no M ࣙ 7.0 events ruptured twice on the same fault segment during the past 2,000 years.
    [Show full text]
  • Seismic Rate Variations Prior to the 2010 Maule, Chile MW 8.8 Giant Megathrust Earthquake
    www.nature.com/scientificreports OPEN Seismic rate variations prior to the 2010 Maule, Chile MW 8.8 giant megathrust earthquake Benoit Derode1*, Raúl Madariaga1,2 & Jaime Campos1 The MW 8.8 Maule earthquake is the largest well-recorded megathrust earthquake reported in South America. It is known to have had very few foreshocks due to its locking degree, and a strong aftershock activity. We analyze seismic activity in the area of the 27 February 2010, MW 8.8 Maule earthquake at diferent time scales from 2000 to 2019. We diferentiate the seismicity located inside the coseismic rupture zone of the main shock from that located in the areas surrounding the rupture zone. Using an original spatial and temporal method of seismic comparison, we fnd that after a period of seismic activity, the rupture zone at the plate interface experienced a long-term seismic quiescence before the main shock. Furthermore, a few days before the main shock, a set of seismic bursts of foreshocks located within the highest coseismic displacement area is observed. We show that after the main shock, the seismic rate decelerates during a period of 3 years, until reaching its initial interseismic value. We conclude that this megathrust earthquake is the consequence of various preparation stages increasing the locking degree at the plate interface and following an irregular pattern of seismic activity at large and short time scales. Giant subduction earthquakes are the result of a long-term stress localization due to the relative movement of two adjacent plates. Before a large earthquake, the interface between plates is locked and concentrates the exter- nal forces, until the rock strength becomes insufcient, initiating the sudden rupture along the plate interface.
    [Show full text]
  • Foreshock Sequences and Short-Term Earthquake Predictability on East Pacific Rise Transform Faults
    NATURE 3377—9/3/2005—VBICKNELL—137936 articles Foreshock sequences and short-term earthquake predictability on East Pacific Rise transform faults Jeffrey J. McGuire1, Margaret S. Boettcher2 & Thomas H. Jordan3 1Department of Geology and Geophysics, Woods Hole Oceanographic Institution, and 2MIT-Woods Hole Oceanographic Institution Joint Program, Woods Hole, Massachusetts 02543-1541, USA 3Department of Earth Sciences, University of Southern California, Los Angeles, California 90089-7042, USA ........................................................................................................................................................................................................................... East Pacific Rise transform faults are characterized by high slip rates (more than ten centimetres a year), predominately aseismic slip and maximum earthquake magnitudes of about 6.5. Using recordings from a hydroacoustic array deployed by the National Oceanic and Atmospheric Administration, we show here that East Pacific Rise transform faults also have a low number of aftershocks and high foreshock rates compared to continental strike-slip faults. The high ratio of foreshocks to aftershocks implies that such transform-fault seismicity cannot be explained by seismic triggering models in which there is no fundamental distinction between foreshocks, mainshocks and aftershocks. The foreshock sequences on East Pacific Rise transform faults can be used to predict (retrospectively) earthquakes of magnitude 5.4 or greater, in narrow spatial and temporal windows and with a high probability gain. The predictability of such transform earthquakes is consistent with a model in which slow slip transients trigger earthquakes, enrich their low-frequency radiation and accommodate much of the aseismic plate motion. On average, before large earthquakes occur, local seismicity rates support the inference of slow slip transients, but the subject remains show a significant increase1. In continental regions, where dense controversial23.
    [Show full text]
  • Earthquake Measurements
    EARTHQUAKE MEASUREMENTS The vibrations produced by earthquakes are detected, recorded, and measured by instruments call seismographs1. The zig-zag line made by a seismograph, called a "seismogram," reflects the changing intensity of the vibrations by responding to the motion of the ground surface beneath the instrument. From the data expressed in seismograms, scientists can determine the time, the epicenter, the focal depth, and the type of faulting of an earthquake and can estimate how much energy was released. Seismograph/Seismometer Earthquake recording instrument, seismograph has a base that sets firmly in the ground, and a heavy weight that hangs free2. When an earthquake causes the ground to shake, the base of the seismograph shakes too, but the hanging weight does not. Instead the spring or string that it is hanging from absorbs all the movement. The difference in position between the shaking part of the seismograph and the motionless part is Seismograph what is recorded. Measuring Size of Earthquakes The size of an earthquake depends on the size of the fault and the amount of slip on the fault, but that’s not something scientists can simply measure with a measuring tape since faults are many kilometers deep beneath the earth’s surface. They use the seismogram recordings made on the seismographs at the surface of the earth to determine how large the earthquake was. A short wiggly line that doesn’t wiggle very much means a small earthquake, and a long wiggly line that wiggles a lot means a large earthquake2. The length of the wiggle depends on the size of the fault, and the size of the wiggle depends on the amount of slip.
    [Show full text]
  • Characteristics of Foreshocks and Short Term Deformation in the Source Area of Major Earthquakes
    Characteristics of Foreshocks and Short Term Deformation in the Source Area of Major Earthquakes Peter Molnar Massachusetts Institute of Technology 77 Massachusetts Avenue Cambridge, Massachusetts 02139 USGS CONTRACT NO. 14-08-0001-17759 Supported by the EARTHQUAKE HAZARDS REDUCTION PROGRAM OPEN-FILE NO.81-287 U.S. Geological Survey OPEN FILE REPORT This report was prepared under contract to the U.S. Geological Survey and has not been reviewed for conformity with USGS editorial standards and stratigraphic nomenclature. Opinions and conclusions expressed herein do not necessarily represent those of the USGS. Any use of trade names is for descriptive purposes only and does not imply endorsement by the USGS. Appendix A A Study of the Haicheng Foreshock Sequence By Lucile Jones, Wang Biquan and Xu Shaoxie (English Translation of a Paper Published in Di Zhen Xue Bao (Journal of Seismology), 1980.) Abstract We have examined the locations and radiation patterns of the foreshocks to the 4 February 1978 Haicheng earthquake. Using four stations, the foreshocks were located relative to a master event. They occurred very close together, no more than 6 kilo­ meters apart. Nevertheless, there appear to have been too clusters of foreshock activity. The majority of events seem to have occurred in a cluster to the east of the master event along a NNE-SSW trend. Moreover, all eight foreshocks that we could locate and with a magnitude greater than 3.0 occurred in this group. The're also "appears to be a second cluster of foresfiocks located to the northwest of the first. Thus it seems possible that the majority of foreshocks did not occur on the rupture plane of the mainshock, which trends WNW, but on another plane nearly perpendicualr to the mainshock.
    [Show full text]
  • PEAT8002 - SEISMOLOGY Lecture 13: Earthquake Magnitudes and Moment
    PEAT8002 - SEISMOLOGY Lecture 13: Earthquake magnitudes and moment Nick Rawlinson Research School of Earth Sciences Australian National University Earthquake magnitudes and moment Introduction In the last two lectures, the effects of the source rupture process on the pattern of radiated seismic energy was discussed. However, even before earthquake mechanisms were studied, the priority of seismologists, after locating an earthquake, was to quantify their size, both for scientific purposes and hazard assessment. The first measure introduced was the magnitude, which is based on the amplitude of the emanating waves recorded on a seismogram. The idea is that the wave amplitude reflects the earthquake size once the amplitudes are corrected for the decrease with distance due to geometric spreading and attenuation. Earthquake magnitudes and moment Introduction Magnitude scales thus have the general form: A M = log + F(h, ∆) + C T where A is the amplitude of the signal, T is its dominant period, F is a correction for the variation of amplitude with the earthquake’s depth h and angular distance ∆ from the seismometer, and C is a regional scaling factor. Magnitude scales are logarithmic, so an increase in one unit e.g. from 5 to 6, indicates a ten-fold increase in seismic wave amplitude. Note that since a log10 scale is used, magnitudes can be negative for very small displacements. For example, a magnitude -1 earthquake might correspond to a hammer blow. Earthquake magnitudes and moment Richter magnitude The concept of earthquake magnitude was introduced by Charles Richter in 1935 for southern California earthquakes. He originally defined earthquake magnitude as the logarithm (to the base 10) of maximum amplitude measured in microns on the record of a standard torsion seismograph with a pendulum period of 0.8 s, magnification of 2800, and damping factor 0.8, located at a distance of 100 km from the epicenter.
    [Show full text]
  • Hypocenter and Focal Mechanism Determination of the August 23, 2011 Virginia Earthquake Aftershock Sequence: Collaborative Research with VA Tech and Boston College
    Final Technical Report Award Numbers G13AP00044, G13AP00043 Hypocenter and Focal Mechanism Determination of the August 23, 2011 Virginia Earthquake Aftershock Sequence: Collaborative Research with VA Tech and Boston College Martin Chapman, John Ebel, Qimin Wu and Stephen Hilfiker Department of Geosciences Virginia Polytechnic Institute and State University 4044 Derring Hall Blacksburg, Virginia, 24061 (MC, QW) Department of Earth and Environmental Sciences Boston College Devlin Hall 213 140 Commonwealth Avenue Chestnut Hill, Massachusetts 02467 (JE, SH) Phone (Chapman): (540) 231-5036 Fax (Chapman): (540) 231-3386 Phone (Ebel): (617) 552-8300 Fax (Ebel): (617) 552-8388 Email: [email protected] (Chapman), [email protected] (Ebel), [email protected] (Wu), [email protected] (Hilfiker) Project Period: July 2013 - December, 2014 1 Abstract The aftershocks of the Mw 5.7, August 23, 2011 Mineral, Virginia, earthquake were recorded by 36 temporary stations installed by several institutions. We located 3,960 aftershocks from August 25, 2011 through December 31, 2011. A subset of 1,666 aftershocks resolves details of the hypocenter distribution. We determined 393 focal mechanism solutions. Aftershocks near the mainshock define a previously recognized tabular cluster with orientation similar to a mainshock nodal plane; other aftershocks occurred 10-20 kilometers to the northeast. Detailed relocation of events in the main tabular cluster, and hundreds of focal mechanisms, indicate that it is not a single extensive fault, but instead is comprised of at least three and probably many more faults with variable orientation. A large percentage of the aftershocks occurred in regions of positive Coulomb static stress change and approximately 80% of the focal mechanism nodal planes were brought closer to failure.
    [Show full text]
  • Earthquake Location Accuracy
    Theme IV - Understanding Seismicity Catalogs and their Problems Earthquake Location Accuracy 1 2 Stephan Husen • Jeanne L. Hardebeck 1. Swiss Seismological Service, ETH Zurich 2. United States Geological Survey How to cite this article: Husen, S., and J.L. Hardebeck (2010), Earthquake location accuracy, Community Online Resource for Statistical Seismicity Analysis, doi:10.5078/corssa-55815573. Available at http://www.corssa.org. Document Information: Issue date: 1 September 2010 Version: 1.0 2 www.corssa.org Contents 1 Motivation .................................................................................................................................................. 3 2 Location Techniques ................................................................................................................................... 4 3 Uncertainty and Artifacts .......................................................................................................................... 9 4 Choosing a Catalog, and What to Expect ................................................................................................ 25 5 Summary, Further Reading, Next Steps ................................................................................................... 30 Earthquake Location Accuracy 3 Abstract Earthquake location catalogs are not an exact representation of the true earthquake locations. They contain random error, for example from errors in the arrival time picks, as well as systematic biases. The most important source of systematic
    [Show full text]
  • Qt88c3k67v.Pdf
    UC Berkeley UC Berkeley Previously Published Works Title Early aftershocks and afterslip surrounding the 2015 Mw 8.4 Illapel rupture Permalink https://escholarship.org/uc/item/88c3k67v Authors Huang, H Xu, W Meng, L et al. Publication Date 2017 DOI 10.1016/j.epsl.2016.09.055 Peer reviewed eScholarship.org Powered by the California Digital Library University of California Early aftershocks and afterslip surrounding the 2015 Mw 8.4 Illapel rupture Author links open overlay panel HuiHuang a WenbinXu bc LingsenMeng a RolandBürgmann b Juan CarlosBaez d Show more https://doi.org/10.1016/j.epsl.2016.09.055 Get rights and content Highlights • Missing early aftershocks and repeaters are recovered by the matched- filtermethod. • Differential southward and northward expansion of early aftershocks are observed. • Repeaters and geodetic data reveal afterslip around the Illapel mainshock rupture. Abstract On 16 September 2015, the Mw 8.4 Illapel earthquake ruptured a section of the subduction thrust on the west coast of central Chile. The mainshock was followed by numerous aftershocks including some normal-faulting events near the trench. We apply a template matching approach to improve the completeness of early aftershocks within one month of the mainshock. To constrain the distribution of afterslip, we utilize repeating earthquakes among the aftershocks and perform a joint slip inversion of postseismic GPS and InSAR data. The results show that the aftershock zone abruptly expands to the south ∼14 h after the mainshock while growing relatively continuously to the north within the first day. The repeating earthquakes accompanying the early expansion suggest that aseismic afterslip on the subduction thrust surrounding the coseismic rupture is an important triggering mechanism of aftershocks in addition to stress transfer or poroelastic effects.
    [Show full text]
  • Mamuju–Majene
    Supendi et al. Earth, Planets and Space (2021) 73:106 https://doi.org/10.1186/s40623-021-01436-x EXPRESS LETTER Open Access Foreshock–mainshock–aftershock sequence analysis of the 14 January 2021 (Mw 6.2) Mamuju–Majene (West Sulawesi, Indonesia) earthquake Pepen Supendi1* , Mohamad Ramdhan1, Priyobudi1, Dimas Sianipar1, Adhi Wibowo1, Mohamad Taufk Gunawan1, Supriyanto Rohadi1, Nelly Florida Riama1, Daryono1, Bambang Setiyo Prayitno1, Jaya Murjaya1, Dwikorita Karnawati1, Irwan Meilano2, Nicholas Rawlinson3, Sri Widiyantoro4,5, Andri Dian Nugraha4, Gayatri Indah Marliyani6, Kadek Hendrawan Palgunadi7 and Emelda Meva Elsera8 Abstract We present here an analysis of the destructive Mw 6.2 earthquake sequence that took place on 14 January 2021 in Mamuju–Majene, West Sulawesi, Indonesia. Our relocated foreshocks, mainshock, and aftershocks and their focal mechanisms show that they occurred on two diferent fault planes, in which the foreshock perturbed the stress state of a nearby fault segment, causing the fault plane to subsequently rupture. The mainshock had relatively few after- shocks, an observation that is likely related to the kinematics of the fault rupture, which is relatively small in size and of short duration, thus indicating a high stress-drop earthquake rupture. The Coulomb stress change shows that areas to the northwest and southeast of the mainshock have increased stress, consistent with the observation that most aftershocks are in the northwest. Keywords: Mamuju–Majene, Earthquake, Relocation, Rupture, Stress-change Introduction mainshock from two of the nearest stations in Mamuju On January 14, 2021, a destructive earthquake (Mw 6.2) and Majene are 95.9 and 92.8 Gals, respectively, equiva- between Mamuju and Majene, West Sulawesi, Indonesia, lent to VI on the MMI scale (Additional fle 1: Figure S1).
    [Show full text]
  • Stress Relaxation Arrested the Mainshock Rupture of the 2016
    ARTICLE https://doi.org/10.1038/s43247-021-00231-6 OPEN Stress relaxation arrested the mainshock rupture of the 2016 Central Tottori earthquake ✉ Yoshihisa Iio 1 , Satoshi Matsumoto2, Yusuke Yamashita1, Shin’ichi Sakai3, Kazuhide Tomisaka1, Masayo Sawada1, Takashi Iidaka3, Takaya Iwasaki3, Megumi Kamizono2, Hiroshi Katao1, Aitaro Kato 3, Eiji Kurashimo3, Yoshiko Teguri4, Hiroo Tsuda5 & Takashi Ueno4 After a large earthquake, many small earthquakes, called aftershocks, ensue. Additional large earthquakes typically do not occur, despite the fact that the large static stress near the edges of the fault is expected to trigger further large earthquakes at these locations. Here we analyse ~10,000 highly accurate focal mechanism solutions of aftershocks of the 2016 Mw 1234567890():,; 6.2 Central Tottori earthquake in Japan. We determine the location of the horizontal edges of the mainshock fault relative to the aftershock hypocentres, with an accuracy of approximately 200 m. We find that aftershocks rarely occur near the horizontal edges and extensions of the fault. We propose that the mainshock rupture was arrested within areas characterised by substantial stress relaxation prior to the main earthquake. This stress relaxation along fault edges could explain why mainshocks are rarely followed by further large earthquakes. 1 Disaster Prevention Research Institute, Kyoto University, Gokasho Uji, Japan. 2 Institute of Seismology and Volcanology, Faculty of Sciences, Kyushu University, Fukuoka, Japan. 3 Earthquake Research Institute, University of
    [Show full text]