Ocean Bottom Seismometer Study of the Kuril Trench Area

Total Page:16

File Type:pdf, Size:1020Kb

Ocean Bottom Seismometer Study of the Kuril Trench Area Zol NOAA-JTRE-166 07 REi OVE HIG-76-9 -- - -· -~ - -· - --' OCEAN BOTTOM SEISMOMETER STUDY ·' OF THE KURil TRENCH AREA By JUNZO KASAHARA and ROBERT R. HARVEY .. ' I 1 / ; . i . AUGUST 1976 . , .. •. HAWAII INSTITUTE OF GEOPHYSICS UNIVERSITY OF HAWAII, HONOLULU and JOI NT TSUNAMI RESEARCH EF FORT PACIFIC MARINE ENVIRONMENTAL LABORATORY ENVIRONMENTAL RESEARCH LABORATORIES, NOAA Distribution of this document is unlimited. Reproduction of this report in whole or in part is permitted for any purpose of the United States Government. HAWAII INSTITUTE OF GEOPHYSICS UNIVERSITY OF HAWAII ·. NOM-JTRE-166 HIG-76-9 OCEAN BOTTOM SEISMOMETER STUDY OF THE KURIL TRENCH AREA By Junzo Kasahara 1 and Robert R. Harvey AUGUST 1976 Hawaii Institute of Geophysics University of Hawaii, Honolulu and Joint Tsunami Research Effort Pacific Marine Environmental Laboratory Environmental Research Laboratories, NOM ~~uJ Director Director Joint Tsunami Research Effort Hawaii Institute Partial support for this research was contributed by Office of Naval Research contract N00014-75-C-0209. 1 ON LEAVE FROM EARTHQUAKE RESEARCH INSTITUTE, UNIVERSITY OF TOKYO. I i - ! ABSTRACT An ocean bottom seismograph was deployed on the seaward side of the Kuril Trench off Hokkaido ~ Japan in 5460 m of water~ in llugust during the 1975 Joint Soviet-American Tsunami Expedition. During the seven- day record" S-P times were distributed in three groups : 19- 24 sec ~ corresponding to aftershocks of the 10 June and 13 June 19?5 earthquakes southeast of Nemuro ~ Japan and to earthquakes east of Sanriku~ Japan; rv30 sec ~ from south of Erimo Peninsula ~ Hokkaido ; and rv100 sec~ from the Izu-Bonin Islands . Seven earthquakes ~ with hypocenters well determined by the land seismic net~ are studied in detail . A shallow focus earthquake yields typical oceanic mantle velocities shallower than 50 km in the slab which dips unde r the Japanese archipelago. However" I ! deeper foc~s earthquakesreveal anomalously high velocities (V > 8. 50 km/sec ~ V > 4. 80 km/sec) averaged over the upper p s - I 230 km~ in agreement with the models of Utsu and Oliver and Isacks. Two deep earthquakes" whose paths lie in the Pacific Ocean asthenospher e" suggest a velocity 3% lower than that predicted by Jeffreys - Bullen~ in agreement with the above models . Spectral analysis of S arrivals suggests Q values of 1000-1500 for nearby s earthquakes (S-P < 43 sec) and 4000-6000 for longer distance earth- quakes ~ implying an unusual attenuation mechanism for long travel path~ which enhances the high frequencies . I I TABLE ' OF CONTENTS ABSTRACT iii LIST OF TABLES vi LIST OF FIGURES vii I INTRODUCTION 1 ! OBS DESCRIPTION l I S-P TIME DISTRIBUTION AND TYPICAL FEATURES 4 I I TRAVEL TIME ANOMALY IN THE SEISMIC ZONE · 8 I Q STRUCTURE 13 I OBS NOISE 15 I CONCLUSIONS 17 REFERENCES 19 TABLES unpaged (follow page 24) FIGURES unpaged (follow Table 3) . I I v LIST OF TABLES l. Arrival times, S- P times, and amplitudes of P-, S-, and T-phases for OBS observations duri ng the 1975 Soviet-American Tsunami Expedition. Amplitudes are taken from the vertical, low-gain channel 2. Hypocenter parameters for the seven earthquakes used in the present analysis, determined from U.S . Geological Survey and Japan Meteorological Agency data. Japan Meteorological Agency I · data are in parentheses 3 . Summary of results for the seven earthquakes used in the present analysis. Origin times and focal depths are from the U.S. Geological Survey Epicenter Determination Record i i ... .-........ ... --.-..-.. m:. !.~~·~--~ ___ ., ....... ~ -.. ~, LIST OF FIGURES 1 . Instrument locations during the 1975 Soviet-American Tsunami Expedition . 2 . Pop-up o c ean bot tom seismograph on board the Soviet vessel R. V. Valerian Uryvaev . 3 . Block diagram of ocean bottom seismog raph. 4 . Estimated response curve for geophone, amplifier, tape recording system, and playback system . 5. Playback scheme. Time compression ratios for original OBS tape recording and Hewlett-Pa ckard 3960 playback are 1:400 and 1:200, r espectively. 6 . S- P time distribution for (a) all detected earthquakes and (b) those with S-P time between 0 and 37 seconds. Shaded area indicates those earthquakes a ccompanied by T-phase activity. 7 . Seismograms as displayed on Visicorder. P, P , S, and T denote 1 P- phase arrival on vertical channel , P-phase arrival on horixontal channel, S- phase arriv al and T- phase arrival, respectively. Top and bottom traces are the time channel, with altered wave f orm of the pr i mary 1-se c pu lses containing a BCD code with day, hour, a n d minute information . Earthquakes (c), (g), (h), (j), and (k) show T-phases . Note that the P-phase arrives earlier on the vertical than on the horizontal c hannel for most earthquakes. 8 . Epic entral distribution o f aftershocks of the 10 June and 13 June 1975 earthquakes (after Japan, Hokkaido University, 1976). vii 9. T-phase amplitude versus P and S wave amplitudes as recorded on the low-gain vertical channel for all earthquakes with S-P time between 19 and 24 sec. T-phase generating earthquakes occurred in the aftershock region of the 10 June and 13 June 1975 earth­ quakes and near the Japan Trench. 10 . Chart showing epicenters of the seven earthquakes used in the present analysis, as determined by Japan Meteorological Agency and the U.S. Geological Survey. ll. Schematic ray paths from the hypocenter to the OBS for (a) earth­ quakes with negative travel time anomalies and (b) earthquakes with normal arrivals. The ray path for (a) lies entirely in the high velocity (HV) , high Q (HQ) zone, whereas for (b), the path lies predominantly in the low vel ocity (LV), low Q (LQ) zone. 12. S- P time versus P arrival t i me for the OBS, vertical channel, using U.S. Geological Survey epicenter determinations. 13. S-P time versus P arrival time for individual earthquakes~ using U. S. Geologi cal Survey epicenter determinations. Land station arrivals are denoted by circles , OBS arrivals by squares. 14. Travel time curves for earthquakes with early OBS arrivals. Land station arrivals are denoted by circles, OBS arrivals by squares. The solid lines represent standard Jeffreys-Bullen travel time curves . 15. Travel time curves for earthquakes with normal OBS arrivals. Symbols are the same as in Fig. 14. 16 . Crustal model used to calculate average mantle velocities, based on the results of Lw:iJJJig et al. [1966] and Den et al. [1971). viii 17. Sonograms as recorded on Sona-Graph. Contours correspond to 6-dh amplitude intervals P, S, and T refer to P- phase, S-phase, and T- phase arrivals; and Hand V refer to horizontal and vertical channels. 18. S-wave spectra for selected earthquakes, obtained as a cut through a sonogram at the peak in S-phase energy and corrected for the ' OBS system response. Numbers on curves refer to S-P time in seconds. 19. Q variation as a function of S-P time. The ordinate refers to the slope of logarithmic amplitude decay with frequency. The solid and dotted lines are calculated using a model with a flat velocity amplitude source spectrum with varying Q for P and S waves, respectively. INTRODUCTION The 1975 Soviet-American Tsunami Expedition i~tended to s tudy tsunami generation, propagat i on, and runup. The program comp ris ed a cooperative e ffort b e tween scientists of the Joint Tsunami Re s earch Ef f ort, NOAA; Hawaii Institute of Geophysics , Uni versit y of Hawaii; and the Sakhalin Complex Scientific Research I nstitute and the Hydrometeorological Service of the U.S.S.R. The field effort [ Soloviev ~ Miller et a l .~ 1976] involved a two-month cruise a long the PaciEi c coast of Hokkaido and the southern Kuril Islands , duri ng whi ch the f ollowing f ree-vehicle instruments were deployed : nine bottom pressure r e corders, one vertical electric f ield recorder, and one ocean bott om seismograph (OBS). Figure 1 s hows the i nstrument locations. This pa per reports on the analysis of t he OBS da ta. Water wave results are being published separ:'ltely [Efimov et a l. ~ in press]. OBS DESC RIPTION The OBS was built at t he Hawaii Institute of Geophysics and is a mo dified ve rsi on of that designed by the Earthquake Research l ns t j Lut e , Un iversi t:y of Tokyo [Ka .s ahm'a et; al . ~ 1973, 1974a, 1974b; 2 Sut t on et al.. ]. The instrument operates as a free vehicle and consists basically of data acquisition and recovery systems . 2 S UT TON , G . H., J . KA S AHA R A, W. N. ICHINOSE, ANO D. A. BYRNE . MS, OCEAN B OTTOM S EISMOGRAPH DEVEL OPMENT AT HAWAII IN S TITUTE OF GEOPHYSICS, IN PR EP ARATI ON, 2 Figure 2 depicts the assembled OBS. Obvious components f rom top to bottom are the flotation module, pressure case, release, and d ispos able ~nchor. Fl ota tio n consists of five 10- inch diameter g lass spheres which provide 8 kg o f net positive buoyancy upon release of the ballast . The 18-cm outside diameter aluminum pressure vessel :is fabric ated of 7075-T6 alloy and is capable of resisting external pressure to 10-km water depth. Dual explos ive bolts separate the a nchor from the i n strume nt p a ckage at the preset release time, which is con tro l led by two independent clocks . I n the photograph a safety shield covers the release mechanism. Fina l l~ a 45-kg core weight serves as ballast; the complete assembly weighs 37 kg in water and sinks at roughly 1 m/sec.
Recommended publications
  • Keck Combined Strong-Motion/Broadband Obs
    KECK COMBINED STRONG-MOTION/BROADBAND OBS WHOI Ocean Bottom Seismograph Laboratory W.M. Keck Foundation Award to Understand Earthquake Predictability at East Pacific Rise Transform Faults. • In 2006, the W.M. Keck Foundation awarded funding to Jeff McGuire and John Collins to determine the physical mechanisms responsible for the observed capability to predict, using foreshocks, large (Mw ~6) transform-fault earthquakes at the East Pacific Rise, and to gain greater insight into the fundamentals of earthquake mechanics in general. • Achieving this objective required building 10 OBS of a new and unique type that could record, without saturation, the large ground motions generated by moderate to large earthquakes at distances of less than ~10 km. W.M. Keck OBS: Combined Broadband Seismometer and Strong-Motion Accelerometer • The broadband OBS available from OBSIP carry a broadband seismometer whose performance is optimized to resolve the earth’s background noise, which can be as small as 10-11 g r.m.s. in a bandwidth of width 1/6 decade at periods of about 100 s. Thus, these sensors are ideal for resolving ground motions from large distant earthquakes, necessary for structural seismology studies. • Ground motions from local, moderate to large earthquakes can generate accelerations of up a g or more, which would saturate or clip these sensors. Currently, there are no sensors (or data-loggers) that have a dynamic range to resolve this ~220 dB range of ground motion. • To overcome this limitation, we used Keck Foundation funding to build 10 OBS equipped with both a conventional broadband seismometer and a strong- motion accelerometer with a clip level of 2.5 g.
    [Show full text]
  • Tracking Past Earthquakes in the Sediment Record Testing and Developing Submarine Paleoseismology in the Deep Sea (JTRACK‐Paleoseismology)
    IODP Expedition 386: Japan Trench Paleoseismology TRACKing past earthquakes in the sediment record Testing and developing submarine Paleoseismology in the deep sea (JTRACK‐Paleoseismology) IODP Expedition 386: Japan Trench Paleoseismology Co‐Chief Scientists: Michael Strasser (University of Innsbruck, Austria) Ken Ikehara (Geological Survey of Japan, AIST) Expedition Project Manager: Jez Everest, British Geological Survey Lena Maeda, JAMSTEC (MarE3 Liasion) JpGU 2020 2020-07-12 Michi Strasser IODP Expedition 386: Japan Trench Paleoseismology Short historical and even shorter instrumental records limit our perspective of earthquake maximum magnitude and recurrence Examining prehistoric events preserved in the geological record is essential to understand long‐term history of giant earthquakes JpGU 2020 2020-07-12 Michi Strasser IODP Expedition 386: Japan Trench Paleoseismology “Submarine paleoseismology” is a promising approach to investigate deposits from the deep sea, where earthquakes leave traces preserved in stratigraphic succession. Submarine paleoseismology study sites (numbers) compiled during Magellan Plus Workshop in Zürich 2015 (McHugh et al., 2016; Strasser et al., 2016) JpGU 2020 2020-07-12 Michi Strasser IODP Expedition 386: Japan Trench Paleoseismology Challenges in Submarine Paleoseismology Can we distinguish different earthquake events and types from the sedimentary records? Is there an earthquake magnitude threshold for a given signal/pattern in the geological record? Does record sensitivity change by margin segmentation, sedimentation and/or through time? Can we link the sedimentary signal to the earthquake rupture characteristics? McHugh et al., 2016; Strasser et al., 2016) JpGU 2020 2020-07-12 Michi Strasser IODP Expedition 386: Japan Trench Paleoseismology IODP is uniquely positioned to provide data by coring sequences comprising continuous depositional conditions and records of earthquakes occurrence over longer time periods.
    [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]
  • BY JOHNATHAN EVANS What Exactly Is an Earthquake?
    Earthquakes BY JOHNATHAN EVANS What Exactly is an Earthquake? An Earthquake is what happens when two blocks of the earth are pushing against one another and then suddenly slip past each other. The surface where they slip past each other is called the fault or fault plane. The area below the earth’s surface where the earthquake starts is called the Hypocenter, and the area directly above it on the surface is called the “Epicenter”. What are aftershocks/foreshocks? Sometimes earthquakes have Foreshocks. Foreshocks are smaller earthquakes that happen in the same place as the larger earthquake that follows them. Scientists can not tell whether an earthquake is a foreshock until after the larger earthquake happens. The biggest, main earthquake is called the mainshock. The mainshocks always have aftershocks that follow the main earthquake. Aftershocks are smaller earthquakes that happen afterwards in the same location as the mainshock. Depending on the size of the mainshock, Aftershocks can keep happening for weeks, months, or even years after the mainshock happened. Why do earthquakes happen? Earthquakes happen because all the rocks that make up the earth are full of fractures. On some of the fractures that are known as faults, these rocks slip past each other when the crust rearranges itself in a process known as plate tectonics. But the problem is, rocks don’t slip past each other easily because they are stiff, rough and their under a lot of pressure from rocks around and above them. Because of that, rocks can pull at or push on each other on either side of a fault for long periods of time without moving much at all, which builds up a lot of stress in the rocks.
    [Show full text]
  • Chapter 2 the Evolution of Seismic Monitoring Systems at the Hawaiian Volcano Observatory
    Characteristics of Hawaiian Volcanoes Editors: Michael P. Poland, Taeko Jane Takahashi, and Claire M. Landowski U.S. Geological Survey Professional Paper 1801, 2014 Chapter 2 The Evolution of Seismic Monitoring Systems at the Hawaiian Volcano Observatory By Paul G. Okubo1, Jennifer S. Nakata1, and Robert Y. Koyanagi1 Abstract the Island of Hawai‘i. Over the past century, thousands of sci- entific reports and articles have been published in connection In the century since the Hawaiian Volcano Observatory with Hawaiian volcanism, and an extensive bibliography has (HVO) put its first seismographs into operation at the edge of accumulated, including numerous discussions of the history of Kīlauea Volcano’s summit caldera, seismic monitoring at HVO HVO and its seismic monitoring operations, as well as research (now administered by the U.S. Geological Survey [USGS]) has results. From among these references, we point to Klein and evolved considerably. The HVO seismic network extends across Koyanagi (1980), Apple (1987), Eaton (1996), and Klein and the entire Island of Hawai‘i and is complemented by stations Wright (2000) for details of the early growth of HVO’s seismic installed and operated by monitoring partners in both the USGS network. In particular, the work of Klein and Wright stands and the National Oceanic and Atmospheric Administration. The out because their compilation uses newspaper accounts and seismic data stream that is available to HVO for its monitoring other reports of the effects of historical earthquakes to extend of volcanic and seismic activity in Hawai‘i, therefore, is built Hawai‘i’s detailed seismic history to nearly a century before from hundreds of data channels from a diverse collection of instrumental monitoring began at HVO.
    [Show full text]
  • Large and Repeating Slow Slip Events in the Izu-Bonin Arc from Space
    LARGE AND REPEATING SLOW SLIP EVENTS IN THE IZU-BONIN ARC FROM SPACE GEODETIC DATA (伊豆小笠原弧における巨大スロー地震および繰り返し スロー地震の宇宙測地学的研究) by Deasy Arisa Department of Natural History Sciences Graduate School of Science, Hokkaido University September, 2016 Abstract The Izu-Bonin arc lies along the convergent boundary where the Pacific Plate subducts beneath the Philippine Sea Plate. In the first half of my three-year doctoral course, I focused on the slow deformation on the Izu Islands, and later in the second half, I focused on the slow deformation on the Bonin Islands. The first half of the study, described in Chapter V, is published as a paper, "Transient crustal movement in the northern Izu–Bonin arc starting in 2004: A large slow slip event or a slow back-arc rifting event?". Horizontal velocities of continuous Global Navigation Satellite System (GNSS) stations on the Izu Islands move eastward by up to ~1 cm/year relative to the stable part of the Philippine Sea Plate suggesting active back-arc rifting behind the northern part of the arc. We confirmed the eastward movement of the Izu Islands explained by Nishimura (2011), and later discussed the sudden accelerated movement in the Izu Islands detected to have occurred in the middle of 2004. I mainly discussed this acceleration and make further analysis to find out the possible cause of this acceleration. Here I report that such transient eastward acceleration, starting in the middle of 2004, resulted in ~3 cm extra movements in three years. I compare three different mechanisms possibly responsible for this transient movement, i.e. (1) postseismic movement of the 2004 September earthquake sequence off the Kii Peninsula far to the west, (2) a temporary activation of the back-arc rifting to the west dynamically triggered by seismic waves from a nearby earthquake, and (3) a large slow slip event in the Izu-Bonin Trench to the east.
    [Show full text]
  • Fully-Coupled Simulations of Megathrust Earthquakes and Tsunamis in the Japan Trench, Nankai Trough, and Cascadia Subduction Zone
    Noname manuscript No. (will be inserted by the editor) Fully-coupled simulations of megathrust earthquakes and tsunamis in the Japan Trench, Nankai Trough, and Cascadia Subduction Zone Gabriel C. Lotto · Tamara N. Jeppson · Eric M. Dunham Abstract Subduction zone earthquakes can pro- strate that horizontal seafloor displacement is a duce significant seafloor deformation and devas- major contributor to tsunami generation in all sub- tating tsunamis. Real subduction zones display re- duction zones studied. We document how the non- markable diversity in fault geometry and struc- hydrostatic response of the ocean at short wave- ture, and accordingly exhibit a variety of styles lengths smooths the initial tsunami source relative of earthquake rupture and tsunamigenic behavior. to commonly used approach for setting tsunami We perform fully-coupled earthquake and tsunami initial conditions. Finally, we determine self-consistent simulations for three subduction zones: the Japan tsunami initial conditions by isolating tsunami waves Trench, the Nankai Trough, and the Cascadia Sub- from seismic and acoustic waves at a final sim- duction Zone. We use data from seismic surveys, ulation time and backpropagating them to their drilling expeditions, and laboratory experiments initial state using an adjoint method. We find no to construct detailed 2D models of the subduc- evidence to support claims that horizontal momen- tion zones with realistic geometry, structure, fric- tum transfer from the solid Earth to the ocean is tion, and prestress. Greater prestress and rate-and- important in tsunami generation. state friction parameters that are more velocity- weakening generally lead to enhanced slip, seafloor Keywords tsunami; megathrust earthquake; deformation, and tsunami amplitude.
    [Show full text]
  • Mw9- Class Earthquakes Versus Smaller Earthquakes and Other Driving Mechanisms
    Expedition Co-chief Scientists Prof. Michael Strasser Michael Strasser is a professor in sedimentary geology at the University of Innsbruck in Austria. His research focuses on the quantitative characterization of dynamic sedimentary and tectonic processes and related geohazards, as unraveled from the event-stratigraphic record of lakes and ocean margins. “Michi” has participated in 5 ocean drilling expeditions to subduction zones (including Nankai Trough Seismogenic Zone The Japan Trench Experiment Expedition 338 as Co-chief) and has received the 2017 AGU/JpGU Asahiko Taira International Scientific Ocean Paleoseismology Drilling Research Prize for his outstanding contributions 6 3 to the investigation of submarine mass movements using Deposit (x 10 m ) multidisciplinary approaches through scientific ocean drilling. Expedition His work on submarine paleoseismology has focused on the Japan Trench since the 2011 Tohoku-oki earthquake, Volume 70 after which he lead two research cruises to characterize the offshore impact of the earthquake on the hadal sedimentary environment. Dr. Ken Ikehara Error Ken Ikehara is a prime senior researcher in the Research Institute of Geology 60 and Geoinformation, Geological Survey of Japan, AIST. His research focuses Mid-value on sedimentology and marine geology of active margins, with special interests in sedimentary processes, formation and preservation of event deposits, Quaternary paleoceanography and Asian monsoon fluctuation. His work on submarine 50 paleoseismology has concentrated not only on the Japan Trench but also on the Nankai Trough, Ryukyu Trench and northern Japan Sea. Ken attended more than 80 survey cruises, mainly around the Japanese islands, including US Sumatra-Andaman Trench, German-Japan Japan Trench, 2000 French Antarctic Ocean cruises, and the IODP Exp 346 Asian monsoon.
    [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]
  • Outer-Rise Normal Fault Development and Influence On
    Boston et al. Earth, Planets and Space 2014, 66:135 http://www.earth-planets-space.com/content/66/1/135 FULL PAPER Open Access Outer-rise normal fault development and influence on near-trench décollement propagation along the Japan Trench, off Tohoku Brian Boston1*, Gregory F Moore1, Yasuyuki Nakamura2 and Shuichi Kodaira2 Abstract Multichannel seismic reflection lines image the subducting Pacific Plate to approximately 75 km seaward of the Japan Trench and document the incoming plate sediment, faults, and deformation front near the 2011 Tohoku earthquake epicenter. Sediment thickness of the incoming plate varies from <50 to >600 m with evidence of slumping near normal faults. We find recent sediment deposits in normal fault footwalls and topographic lows. We studied the development of two different classes of normal faults: faults that offset the igneous basement and faults restricted to the sediment section. Faults that cut the basement seaward of the Japan Trench also offset the seafloor and are therefore able to be well characterized from multiple bathymetric surveys. Images of 199 basement-cutting faults reveal an average throw of approximately 120 m and average fault spacing of approximately 2 km. Faults within the sediment column are poorly documented and exhibit offsets of approximately 20 m, with densely spaced populations near the trench axis. Regional seismic lines show lateral variations in location of the Japan Trench deformation front throughout the region, documenting the incoming plate’s influence on the deformation front’s location. Where horst blocks are carried into the trench, seaward propagation of the deformation front is diminished compared to areas where a graben has entered the trench.
    [Show full text]
  • Repeated Occurrence of Surface-Sediment Remobilization
    Ikehara et al. Earth, Planets and Space (2020) 72:114 https://doi.org/10.1186/s40623-020-01241-y FULL PAPER Open Access Repeated occurrence of surface-sediment remobilization along the landward slope of the Japan Trench by great earthquakes Ken Ikehara1* , Kazuko Usami1,2 and Toshiya Kanamatsu3 Abstract Deep-sea turbidites have been utilized to understand the history of past large earthquakes. Surface-sediment remo- bilization is considered to be a mechanism for the initiation of earthquake-induced turbidity currents, based on the studies on the event deposits formed by recent great earthquakes, such as the 2011 Tohoku-oki earthquake, although submarine slope failure has been considered to be a major contributor. However, it is still unclear that the surface-sed- iment remobilization has actually occurred in past great earthquakes. We examined a sediment core recovered from the mid-slope terrace (MST) along the Japan Trench to fnd evidence of past earthquake-induced surface-sediment remobilization. Coupled radiocarbon dates for turbidite and hemipelagic muds in the core show small age diferences (less than a few 100 years) and suggest that initiation of turbidity currents caused by the earthquake-induced surface- sediment remobilization has occurred repeatedly during the last 2300 years. On the other hand, two turbidites among the examined 11 turbidites show relatively large age diferences (~ 5000 years) that indicate the occurrence of large sea-foor disturbances such as submarine slope failures. The sedimentological (i.e., of diatomaceous nature and high sedimentation rates) and tectonic (i.e., continuous subsidence and isolated small basins) settings of the MST sedimentary basins provide favorable conditions for the repeated initiation of turbidity currents and for deposition and preservation of fne-grained turbidites.
    [Show full text]
  • 10. Crustal Structure of the Japan Trench
    10. CRUSTAL STRUCTURE OF THE JAPAN TRENCH: THE EFFECT OF SUBDUCTION OF OCEAN CRUST Sandanori Murauchi, Department of Earth Sciences, Chiba University, Chiba, Japan and William J. Ludwig, Lamont-Doherty Geological Observatory of Columbia University, Palisades, New York ABSTRACT Evaluation and synthesis of seismic-refraction measurements made in the Japan trench in the light of the results of deep-sea drill- ing from Glomar Challenger Legs 56 and 57 result in a schematic sec- tion of the crustal structure. The Pacific Ocean crustal plate under- thrusts the leading edge of the continental block of Northeast Japan at a low angle and follows at depth the upper seismic belt of the Wadati-Benioff zone. Overthrust continental crust extends to within 30 km of the trench axis; thenceforward the lower inner trench slope is formed by a thick, wedge-shaped body of low-velocity sediments. The volume of these sediments is too small to represent all the sedi- ments scraped off the Pacific plate and transported from land. This indicates that substantial amounts of sediment are carried down along slip planes between the continental block and the descending plate. Dewatering of the sediments lubricates the slip planes. The slip planes migrate upward into the overlying continental edge, causing removal of material from its base. This tectonic erosion causes sub- sidence and landward retreat of the continental edge. INTRODUCTION between 39 and 40° N. Lines of multichannel seismic- reflection measurements were made by JAPEX to select In terms of plate tectonics, the convergence of two the prime drill sites (see foldouts, back cover, this crustal plates may result in underthrusting (subduction) volume, Part 1; Nasu et al., 1979).
    [Show full text]