Hypothesis Tests on Rayleigh Wave Radiation Pattern Shapes: a Theoretical Assessment of Idealized Source Screening

Total Page:16

File Type:pdf, Size:1020Kb

Hypothesis Tests on Rayleigh Wave Radiation Pattern Shapes: a Theoretical Assessment of Idealized Source Screening Geophys. J. Int. (2021) 225, 1653–1671 doi: 10.1093/gji/ggab055 Advance Access publication 2021 February 10 GJI Seismology Hypothesis tests on Rayleigh wave radiation pattern shapes: a theoretical assessment of idealized source screening Joshua D. Carmichael Joshua D Carmichael EES-17, Los Alamos National Laboratory, P.O. Box 1663,MSD446, Los Alamos, NM 87545, USA. E-mail: [email protected] Accepted 2021 February 8. Received 2021 January 31; in original form 2020 September 16 Downloaded from https://academic.oup.com/gji/article/225/3/1653/6132273 by guest on 25 September 2021 SUMMARY Shallow seismic sources excite Rayleigh wave ground motion with azimuthally dependent radiation patterns. We place binary hypothesis tests on theoretical models of such radiation patterns to screen cylindrically symmetric sources (like explosions) from non-symmetric sources (like non-vertical dip-slip or non-VDS faults). These models for data include sources with several unknown parameters, contaminated by Gaussian noise and embedded in a layered half-space. The generalized maximum likelihood ratio tests that we derive from these data models produce screening statistics and decision rules that depend on measured, noisy ground motion at discrete sensor locations. We explicitly quantify how the screening power of these statistics increase with the size of any dip-slip and strike-slip components of the source, relative to noise (faulting signal strength) and how they vary with network geometry. As applications of our theory, we apply these tests to (1) find optimal sensor locations that maximize the probability of screening non-circular radiation patterns and (2) invert for the largest non- VDS faulting signal that could be mistakenly attributed to an explosion with damage, at a particular attribution probability. Finally, we quantify how certain errors that are sourced by opening cracks increase screening rate errors. While such theoretical solutions are ideal and require future validation, they remain important in underground explosion monitoring scenarios because they provide fundamental physical limits on the discrimination power of tests that screen explosive from non-VDS faulting sources. Key words: Theoretical seismology; Surface waves and free oscillations; Earthquake moni- toring and test-ban treaty verification; Probability distributions. ‘faulting signal’ on the radiation pattern shape is significantly non- 1 INTRODUCTION circular or has a low signal-to-noise ratio (SNR). Smaller yield ex- Seismic sources produce Rayleigh wave radiation patterns that indi- plosions (∼101−103kg) that do not trigger tectonic release may still cate focal mechanism asymmetry (Fig. 1). Teleseismic and regional accompany fracturing events or mechanical sliding on rock joints records of large underground nuclear explosions (∼101−103kT) that output shear energy as bulk damage (Steedman et al. 2016). emplaced in pre-stressed geologies, for example, have historically These bulk effects do not appear to significantly distort surface revealed that tectonic release of strain can superimpose with the wave radiation patterns when they are symmetric about a vertical isotropic explosion source to produce Love and Rayleigh waves axis. In particular, local distance records from a series of conven- with non-circular radiation patterns (Toksoz¨ & Kehrer 1972;Ek- tional explosives conducted through the source physics experiment strom¨ & Richards 1994). These observations contrast with simple (SPE, Snelson et al. 2013) demonstrate that low yield, shallowly models of cylindrically symmetric, shallow sources hosted in verti- buried sources that cause damage are vertical-axis symmetric, and cally stratified geologies that predict azimuthally constant Rayleigh thereby trigger Rayleigh wave radiation patterns that are circular wave amplitudes and absent Love waves. Instead, such observa- within a factor of 1.25 (Larmat et al. 2017). These explosions, tions are partially consistent with models of faulting motion pre- which were emplaced in the granites of Climax stock on the Nevada sented by tectonic release, which produces asymmetric deformation National Security Site (NNSS), also demonstrate that body waves about a vertical axis that excites a Rayleigh-wave field with a non- radiated by the same source in a similar frequency band show ap- circular radiation pattern (Richards & Ekstrom¨ 1995). Observers parent azimuthally asymmetry that is likely sourced by refraction risk misidentifying large, shallow explosions that accompany such effects (Darrh et al. 2019). Experiments with low-yield explosives tectonic release as shallow earthquakes when the imprint of such a emplaced in boreholes within New Hampshire granite demonstrate C The Author(s) 2021. Published by Oxford University Press on behalf of The Royal Astronomical Society. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited. 1653 1654 J.D. Carmichael Downloaded from https://academic.oup.com/gji/article/225/3/1653/6132273 by guest on 25 September 2021 Figure 1. Surface sensors (triangles) record Rayleigh waves from a shallow explosion that is buried to a depth h in a horizontally-stratified half-space that has moment MI, which creates damage with moment MCLVD that each superimpose with faulting of moment M0. The damage occurs when constructive interference between the incident and reflected waves create a conically shaped zone of failure. (a) An explosion source capable of producing damage that is symmetric about a vertical axis, but that includes no faulting (no tectonic release) radiates a circular radiation pattern REX described at top. (b) A source that includes non-VDS faulting near the explosion point radiates a non-circular radiation pattern REQ described at top. Each radiation pattern shape associates with a deterministic scalar (bottom) that quantifies the power of the hypothesis test between data that record circular versus non-circular radiation patterns (at top). Section 4.1 defines each symbol. more complex effects. Namely, these latter experiments reveal that is therefore more earthquake-like than explosion-like. A discrimi- observationally confirmed radial fracturing in hard rock accom- nant that tests radiation pattern distortion from local to teleseismic panies asymmetric, short period (∼6 Hz), guided Rayleigh waves ranges can therefore benefit both the source physics community (Rg). Body waves sourced by these same New Hampshire explo- and support nuclear test-ban treaty surveillance, if justified on both sions can exhibit even greater azimuthal dependence (Stroujkova theoretical and experimental grounds. 2018). This work determines if a discriminant for shallow source types Both the SPE and New Hampshire experiments cumulatively in- that tests Rayleigh wave radiation pattern shapes is justified on dicate two substantive effects of the seismic source on radiation theoretical grounds. To confront this challenge, we apply binary hy- pattern shape can be observed from local distances. First, verti- pothesis tests to competing data models of noisy radiation patterns cal axis-symmetric damage does not significantly distort Rayleigh and assume several source parameters are unknown. Our models wave radiation pattern shapes from circularity, whereas a struc- also use planar geologies and therefore isotropic propagation of ture at depth can distort body wave patterns. Secondly, signifi- Rayleigh waves; we do not consider Love waves. Under this limited cant radial fracturing and shearing motion at the shallow explo- scope, we derive screening curves from the hypothesis tests that sion source measurably distorts both Rayleigh wave and body bound an observers’s capability to discriminate non-vertical dip- wave radiation patterns. These observations indicate that az- slip (non-VDS) shallow faulting sources from symmetric sources imuthal variability of Rayleigh waves sourced by small yield ex- (like shallow explosions that create damage that is symmetric about plosions indicate faulting or shearing motion at the source, whereas a vertical axis). The screening power of these tests is completely body wave asymmetry appears non-uniquely attributed to source defined by the product of a faulting-signal term, and a term that and path. depends on deployment parameters. Using this test, we illustrate A forthcoming test within the SPE series will provide a unique op- several applications of our theory that include finding deployment portunity to study asymmetry in radiation patterns that are sourced locations for sensors to supplement an existing network and that by explosions and superimposed with historic, tectonic records of maximize our source-type screening probability. We conclude that fault slip. This effort will detonate a conventional explosive in a Rayleigh wave radiation pattern discriminant shows a high proba- tectonic regions and monitor its seismic signatures for compari- bility PrD of success (PrD > 0.9) when a sufficient number of sensors son against earlier earthquake signatures that output radiation that (>12) with a limited azimuthal gap (<90◦) records radiation from shares wavefront paths (Walter et al. 2012). If Rayleigh waves out- sources with moderate strike-slip faulting signals (SNR >20). This put by this explosion remains circular and mismatches historical probability diminishes with more ambiguous focal
Recommended publications
  • Deep Dehydration As a Plausible Mechanism of the 2013 Mw 8.3 Sea of Okhotsk Deep-Focus Earthquake
    ORIGINAL RESEARCH published: 04 August 2021 doi: 10.3389/feart.2021.521220 Deep Dehydration as a Plausible Mechanism of the 2013 Mw 8.3 Sea of Okhotsk Deep-Focus Earthquake Hao Zhang 1,2*, Suzan van der Lee 2, Craig R. Bina 2 and Zengxi Ge 3 1University of Utah Seismograph Stations, University of Utah, Salt Lake City, UT, United States, 2Department of Earth and Planetary Sciences, Northwestern University, Evanston, IL, United States, 3School of Earth and Space Sciences, Peking University, Beijing, China The rupture mechanisms of deep-focus (>300 km) earthquakes in subducting slabs of oceanic lithosphere are not well understood and different from brittle failure associated with shallow (<70 km) earthquakes. Here, we argue that dehydration embrittlement, often invoked as a mechanism for intermediate-depth earthquakes, is a plausible alternative model for this deep earthquake. Our argument is based upon the orientation and size of the plane that ruptured during the deep, 2013 Mw 8.3 Sea of Okhotsk earthquake, its rupture velocity and radiation efficiency, as well as diverse evidence of water subducting as deep as the transition zone and below. The rupture process of this earthquake has been inferred from back-projecting dual-band seismograms recorded at hundreds of seismic stations in North America and Europe, as well as by fitting P-wave trains recorded at dozens of Edited by: globally distributed stations. If our inferences are correct, the entirety of the subducting Sebastiano D’Amico, fi University of Malta, Malta Paci c lithosphere cannot be completely dry at deep, transition-zone depths, and other Reviewed by: deep-focus earthquakes may also be associated with deep dehydration reactions.
    [Show full text]
  • Large Intermediate-Depth Earthquakes and the Subduction Process
    80 Physics ofthe Earth and Planetary Interiors, 53 (1988) 80—166 Elsevier Science Publishers By., Amsterdam — Printed in The Netherlands Large intermediate-depth earthquakes and the subduction process Luciana Astiz ~, Thorne Lay 2 and Hiroo Kanamori ~ ‘Seismological Laboratory, California Institute of Technology, Pasadena, CA (U.S.A.) 2 Department of Geological Sciences, University ofMichigan, Ann Arbor, MI (USA.) (Received September 22, 1987; accepted October 21, 1987) Astiz, L., Lay, T. and Kanamori, H., 1988. Large intermediate-depth earthquakes and the subduction process. Phys. Earth Planet. Inter., 53: 80—166. This study provides an overview of intermediate-depth earthquake phenomena, placing emphasis on the larger, tectonically significant events, and exploring the relation of intermediate-depth earthquakes to shallower seismicity. Especially, we examine whether intermediate-depth events reflect the state of interplate coupling at subduction zones. and whether this activity exhibits temporal changes associated with the occurrence of large underthrusting earthquakes. Historic record of large intraplate earthquakes (m B 7.0) in this century shows that the New Hebrides and Tonga subduction zones have the largest number of large intraplate events. Regions associated with bends in the subducted lithosphere also have many large events (e.g. Altiplano and New Ireland). We compiled a catalog of focal mechanisms for events that occurred between 1960 and 1984 with M> 6 and depth between 40 and 200 km. The final catalog includes 335 events with 47 new focal mechanisms, and is probably complete for earthquakes with mB 6.5. For events with M 6.5, nearly 48% of the events had no aftershocks and only 15% of the events had more than five aftershocks within one week of the mainshock.
    [Show full text]
  • Phantom Earthquakes
    JOURNAL OF GEOPHYSICAL RESEARCH, VOL. ???, XXXX, DOI:10.1029/, Zagros \phantom earthquakes" reassessed | the interplay of seismicity and deep salt flow in the Simply Folded Belt? Edwin Nissen,1 James Jackson,2 Salman Jahani,3 and Mohammad Tatar4 Abstract. Unravelling the contributions of mainshock slip, aftershocks, aseismic after- slip and postseismic relaxation to the deformation observed in earthquake sequences height- ens our understanding of crustal rheology, triggering phenomena and seismic hazard. Here, we revisit two recent earthquakes in the Zagros mountains (Iran) which exhibited un- usual and contentious after-effects. The Mw ∼6 earthquakes at Qeshm (2005) and Fin (2006) are both associated with large InSAR signals, consistent with slip on steep re- verse faults in carbonate rocks of the middle sedimentary cover, but small aftershocks detected with local seismic networks were concentrated at significantly greater depths. This discrepancy can be interpreted in one of two ways: either (1) there is a genuine ver- tical separation between mainshock and aftershocks, reflecting a complex stress state near the basement{cover interface; or (2) the aftershocks delimit the mainshock slip and the InSAR signals were caused by shallow, up-dip afterslip (\phantom earthquakes") with very similar magnitudes, mechanisms and geographical positions as the original earth- quakes. Here, we show that mainshock centroid depths obtained from body-waveform modelling | which in this instance is the only method that can reveal for certain the depth at which seismic slip was centered | strongly support the first interpretation. At Qeshm, microseismic aftershock depths are centered at the level of the Hormuz Forma- tion, an Infracambrian sequence of intercalated evaporitic and non-evaporitic sediments.
    [Show full text]
  • Nissen-Etal-2010-EPS
    Earth and Planetary Science Letters 296 (2010) 181–194 Contents lists available at ScienceDirect Earth and Planetary Science Letters journal homepage: www.elsevier.com/locate/epsl The vertical separation of mainshock rupture and microseismicity at Qeshm island in the Zagros fold-and-thrust belt, Iran E. Nissen a,⁎, F. Yamini-Fard b, M. Tatar b, A. Gholamzadeh b,1, E. Bergman c, J.R. Elliott d, J.A. Jackson a, B. Parsons d a COMET, Bullard Laboratories, Department of Earth Sciences, University of Cambridge, Madingley Road, Cambridge CB3 0EZ, UK b International Institute of Earthquake Engineering and Seismology, PO Box 19395-3913, Tehran, Iran c Department of Physics, University of Colorado, Boulder, CO 80309-0390, USA d COMET, Department of Earth Sciences, University of Oxford, Parks Road, Oxford OX1 3PR, UK article info abstract Article history: We investigate the depth and geometry of faulting within a cluster of buried, reverse faulting earthquakes Received 11 January 2010 that struck Qeshm island, in the Zagros fold-and-thrust belt, over a four year period between November 2005 Received in revised form 24 March 2010 and July 2009. Of particular interest is our observation that there was a vertical separation between the Accepted 24 April 2010 largest two earthquakes (M 5.8 and 5.9), which ruptured the lower parts of a ∼10-km thick sedimentary Available online 9 June 2010 w cover, and microseismicity recorded by a local network after the first, Mw 5.8 event, which was concentrated – — Editor: T.M. Harrison within the underlying basement at depths of 10 20 km.
    [Show full text]
  • The Mw 7.0 Haiti Earthquake of January 12, 2010: Report #1
    EERI Special Earthquake Report — April 2010 Learning from Earthquakes The Mw 7.0 Haiti Earthquake of January 12, 2010: Report #1 This is the first of multipleNewsletter The EERI contribution was funded Rico to the east and Jamaica and inserts on the Haiti earthquake of by the Learning from Earthquakes Cuba to the west, and has a total January 12, 2010. It summarizes project of the National Science Foun- population of approximately 9 mil- observations from the advance dation under Award #CMMI-0758529. lion. Its largest city, Port-au-Prince, team organized by the U.S. Geo- with an estimated population of be- logical Survey (USGS) and EERI Introduction tween 2.5 and 3 million people, is that traveled to Haiti January 26 to located 25 km ENE of the epicen- The Mw 7.0 earthquake that struck February 3, 2010. The multidiscip- ter. Haiti is the poorest country in the Republic of Haiti on January 12, linary team included Marc Eberhard, the Western Hemisphere, with an 2010, is among the most destructive University of Washington (team estimated 80% of its people living earthquakes in recorded history. As leader); Steve Baldridge, Baldridge under the poverty line, 54% in ab- of March 2010, the death toll report- & Associates Structural Engineer- ject poverty (CIA, 2010). In 2008, ed by the Government of Haiti ex- ing, Inc.; Justin Marshall, Auburn more than 800 people were killed ceeded 233,000, with an additional University; Walter Mooney, USGS; by four hurricanes and tropical 300,000 injuries. More than 5 million and Glenn Rix, Georgia Institute of storms that struck during a two- people live in the area affected by the Technology.
    [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]
  • Complex Rupture During the 12 January 2010 Haiti Earthquake G
    ARTICLES PUBLISHED ONLINE: 10 OCTOBER 2010 | DOI: 10.1038/NGEO977 Complex rupture during the 12 January 2010 Haiti earthquake G. P. Hayes1,2*, R. W. Briggs1, A. Sladen3, E. J. Fielding4, C. Prentice5, K. Hudnut6, P. Mann7, F. W. Taylor7, A. J. Crone1, R. Gold1, T. Ito3,8 and M. Simons3 Initially, the devastating Mw 7.0, 12 January 2010 Haiti earthquake seemed to involve straightforward accommodation of oblique relative motion between the Caribbean and North American plates along the Enriquillo–Plantain Garden fault zone. Here, we combine seismological observations, geologic field data and space geodetic measurements to show that, instead, the rupture process involved slip on multiple faults. Primary surface deformation was driven by rupture on blind thrust faults with only minor, deep, lateral slip along or near the main Enriquillo–Plantain Garden fault zone; thus the event only partially relieved centuries of accumulated left-lateral strain on a small part of the plate-boundary system. Together with the predominance of shallow off-fault thrusting, the lack of surface deformation implies that remaining shallow shear strain will be released in future surface-rupturing earthquakes on the Enriquillo–Plantain Garden fault zone, as occurred in inferred Holocene and probable historic events. We suggest that the geological signature of this earthquake—broad warping and coastal deformation rather than surface rupture along the main fault zone—will not be easily recognized by standard palaeoseismic studies. We conclude that similarly complex earthquakes in tectonic environments that accommodate both translation and convergence—such as the San Andreas fault through the Transverse Ranges of California—may be missing from the prehistoric earthquake record.
    [Show full text]
  • Improving the Determination of Moment Tensors, Moment Magnitudes and Focal Depths of Earthquakes Below Mw 4.0 Using Regional Broadband Seismic Data
    Improving the determination of moment tensors, moment magnitudes and focal depths of earthquakes below Mw 4.0 using regional broadband seismic data: Author: Nawa Dahal Persistent link: http://hdl.handle.net/2345/bc-ir:108624 This work is posted on eScholarship@BC, Boston College University Libraries. Boston College Electronic Thesis or Dissertation, 2019 Copyright is held by the author, with all rights reserved, unless otherwise noted. IMPROVING THE DETERMINATION OF MOMENT TENSORS, MOMENT MAGNITUDES AND FOCAL DEPTHS OF EARTHQUAKES BELOW Mw 4.0 USING REGIONAL BROADBAND SEISMIC DATA NAWA R. DAHAL A dissertation submitted to the Faculty of the Department of Physics in partial fulfillment of the requirements for the degree of Doctor of Philosophy Boston College Morrissey College of Arts and Sciences Graduate School September 2019 © Copyright 2019 Nawa R. Dahal IMPROVING THE DETERMINATION OF MOMENT TENSORS, MOMENT MAGNITUDES AND FOCAL DEPTHS OF EARTHQUAKES BELOW M4.0 USING REGIONAL BROADBAND SEISMIC DATA Author: Nawa R. Dahal Advisors: Prof. Michael J. Naughton and Prof. John E. Ebel Committee Members: Prof. David Broido Prof. Michael Graf ABSTRACT Determining accurate source parameters of small magnitude earthquakes is important to understand the source physics and tectonic processes that activate a seismic source as well as to make more accurate estimates of the probabilities of the recurrences of large earthquakes based on the statistics of smaller earthquakes. The accurate determination of the focal depths and focal mechanisms of small earthquakes is required to constrain the potential seismic source zones of future large earthquakes, whereas the accurate determination of seismic moment is required to calculate the sizes (best represented by moment magnitudes) of earthquakes.
    [Show full text]
  • Source Process and Tectonic Implications of the Great 1975 North Atlantic Earthquake
    Geophys. J. R. astr. SOC.(1985) 82, 497-510 Source process and tectonic implications of the great 1975 North Atlantic earthquake Christopher S. Lynnes and Larry J. Ruff Departmentof Geological Sciences, University of Michigan, Ann Arbor, M148109, USA Accepted 1985 January 28. Received 1985 January28; in original form 1984 August 24 Summary. The Atlantic segment of the Africa-Europe plate boundary has usually been interpreted as a transform boundary on the basis of the bathymetric expression of the Gloria fault and dextral strike-slip first-motion mechanisms aligned along the Azores-Gibraltar line of seismicity. The 1975 May 26 earthquake (Ms=7.9) was assumed to fit into this framework because it occurred in the general area of this line and has a similar first-motion focal mechanism (strike=288", dip=72", slip angle=184"). However, several anomalies cast doubt on this picture: the event is abnormally large for an oceanic transform event; a sizeable tsunami was excited; the aftershock area is unusually small for such a large event; and most significantly, the epicentre is 200 km south of the presumed plate boundary. The Rayleigh wave radiation pattern indicates a change in focal mechanism to one with a significant dip-slip component. The short duration of the source time history (20 s, as deconvolved from long-period P-waves), the lack of directivity in the Rayleigh waves, and the small one-day aftershock area suggest a fault length less than 80 km. One nodal plane of the earthquake is approximately aligned with the trace of an ancient fracture zone. We have compared the Pasadena 1-90 record of the 1975 earthquake to that of the 1941 North Atlantic strike-slip earthquake (200km to the NNW) and confirmed the large size of the 1941 event (M=8.2).
    [Show full text]
  • Focal Mechanism Determination Using High Frequency Waveform Matching and Its Application to Small Magnitude Induced Earthquakes
    Focal Mechanism Determination Using High Frequency Waveform Matching and Its Application to Small Magnitude Induced Earthquakes Junlun Li, Haijiang Zhang, H. Sadi Kuleli, and M. Nafi Toksoz [email protected] Earth Resources Laboratory Department of Earth, Atmospheric and Planetary Sciences Massachusetts Institute of Technology 77 Massachusetts Avenue, Cambridge, MA 02139 1 Summary We present a new method using high frequency full waveform information to determine the focal mechanisms of small, local earthquakes monitored by a sparse surface network. During the waveform inversion, we maximize both the phase and amplitude matching between the observed and modeled waveforms. In addition, we use the polarities of the first P-wave arrivals and the average S/P amplitude ratios to better constrain the matching. An objective function is constructed to include all four criteria. An optimized grid search method is used to search over all possible ranges of source parameters (strike, dip and rake). To speed up the algorithm, a library of Green’s functions is pre-calculated for each of the moment tensor components and possible earthquake locations. Optimizations in filtering and cross-correlation are performed to further speed the grid search algorithm. The new method is tested on a 5-station surface network used for monitoring induced seismicity at a petroleum field. The synthetic test showed that our method is robust and efficient to determine the focal mechanism when using only the vertical component of seismograms in the frequency range of 3 to 9 Hz. The application to dozens of induced seismic events showed satisfactory waveform matching between modeled and observed seismograms.
    [Show full text]
  • Measuring Earthquake Size Earlyideas
    LECTURE 4 MEASURING EARTHQUAKE SIZE EARLYIDEAS •Describe damage inflicted by earthquake →→ "INTENSITY Scales" Always written with roman numerals (IV,VII, XI, etc.) Dynamic connection: Intensity should express ground acceleration BUT... Shortcomings of Intensity Scales •Not directly related to earthquake source •Damage obviously distance-depen- dent •Needs population to report damage •Affected by site response Example of Intensity maps for 1886 Charleston, USA, earthquake. EARTHQUAKE MAGNITUDES →→ •Anessentially empirical concept, intr- •TTo thisot day,his day,measurements have oduced by Richter [1935], long before measurementsremained larhagelyve ad hoc,especially at anyphysical understanding of earth- remainedshort largelydistances. quakesources ad hoc, especially at short distances. [Bolt, 1987] PROGRESS in the 1940s •Apply worldwide •Try (!!) to justify theoretically →→ Leads to first worldwide quantified catalogue of earthquakes "Seismicity of the Earth" Gutenbergand Richter [1944; 1954] B. Gutenberg, 1958 "MODERN" MAGNITUDES Standardized at Prague meeting of the IUGG (1961) •Use Body (P)Wav estodefine short period magnitude, mb around a period of 1 second Q(∆, h) A m = log + Q(∆; h) h b 10 T •Use Surface (Rayleigh)wav e to define = "Long"-period magnitude, Ms,at T 20 seconds A M = log + 1. 66 log ∆+3. 3 s 10 T 10 ∆ Still largely empirical; Constants not justified [Okal, 1989] BODY-WAVE MAGNITUDE mb From first-arriving wave trains (" P "Wav es) *Should be measured at period close to 1 second SUMATRA−ANDAMAN, 26 DEC 2004 Station CTA(Charter Towers, Queensland, Australia); ∆=55° •Remove instrument response •Band-pass filter between 0.3 and 3 seconds •Select windowof80seconds duration around P wave •Apply Body-wav e Magnitude formula A m = log + Q(∆; h)(A in microns) b 10 T mb = 7.
    [Show full text]
  • 1. Introduction
    EARTHQUAKE MAGNITUDE, INTENSITY, ENERGY, POWER LAW RELATIONS AND SOURCE MECHANISM J.R. Kayal Geological Survey of India, 27, J.L. Nehru Road Road, Kolkata – 700 016 email : [email protected] EARTHQUAKE MAGNITUDE Magnitude is one of the basic and important parameters of an earthquake. It defines the size of an earthquake. The beginners of seismology are, in general, confused about different scales of magnitude, and sometimes they mix-up earthquake intensity with its magnitude. Journalists often report the magnitude value of an earthquake as its intensity; this is wrong. There are now different magnitude scales to define the size of an earthquake. After Richter (1935), various magnitude scales are proposed; all these scales are discussed below. Richter Magnitude (or Local Magnitude) ML Richter (1935) defined the local magnitude ML of an earthquake observed at a station to be ML = log A - log Ao ( ∆) (1) where A is the maximum amplitude in millimetres recorded on the Wood- Anderson seismograph for an earthquake at epicentral distance of ∆ km, and Ao (∆ ) is the maximum amplitude at ∆ km for a standard earthquake. The local magnitude is thus a number characteristic of the earthquake, and independent of the location of the recording station. Three arbitrary choices are made in the above definition: (i) the use of standard Wood-Anderson seismograph, (ii) the use of common logarithms to the base 10, and (iii) selection of the standard earthquake whose amplitudes as a function of distance are represented by Ao (∆). The zero level of Ao (∆) can be fixed by choosing its value at a particular distance. Richter chose the zero level of Ao (∆) to be 1 µm (or 0.001 mm) at a distance of 100 km from the earthquake epicentre.
    [Show full text]