The Geophysics, Geology and Mechanics of Slow Fault Slip
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Transform Faults Represent One of the Three
8 Transform faults ransform faults represent one of the three Because of the drift of the newly formed oceanic types of plate boundaries. A peculiar aspect crust away from ridge segments, a relative move- T of their nature is that they are abruptly trans- ment along the faults is induced that corresponds formed into another kind of plate boundary at their to the spreading velocity on both sides of the termination (Wilson, 1965). Plates glide along the ridge. Th e sense of displacement is contrary to fault and move past each other without destruc- the apparent displacement of the ridge segments tion of or creation of new crust. Although crust is (Fig. 8.1b). In the example shown, the transform neither created or destroyed, the transform margin fault is a right-lateral strike-slip fault; if an observer is commonly marked by topographic features like straddles the fault, the right-hand side of the fault scarps, trenches or ridges. moves towards the observer, regardless of which Transform faults occur as several diff erent geo- way is faced. Transform faults end abruptly in a metries; they can connect two segments of growing point, the transformation point, where the strike- plate boundaries (R-R transform fault), one growing slip movement is transformed into a diverging or and one subducting plate boundary (R-T transform converging movement. Th is property gives this fault) or two subducting plate boundaries (T-T fault its name. In the example of the R-R transform transform fault); R stands for mid-ocean ridge, T for fault, the movement at both ends of the fault is deep sea trench ( subduction zone). -
Volcanic Tremor Analysis Based on Advanced Signal Processing Concepts Including Music Information Retrieval (MIR) Strategies
Volcanic tremor analysis based on advanced signal processing concepts including music information retrieval (MIR) strategies Zahra Zali NatRiskChange spring meeting 2019 Outline § Volcanic seismology- Volcanic tremors § Methodology; music processing tools § PhD Project prospect § Examples 2 Volcanic seismology Volcanic seismology represents the main, and often the only, tool to forecast volcanic eruptions and to monitor the eruption process. A seismogram of volcanic earthquakes in an active period gives the general impression of the different types of the seismic signals associated with volcano-tectonic earthquakes, explosions, rock falls, or tremor. Volcanic tremor is often used in conjunction with earthquake swarms as a geophysical warning that an eruption is not far off since it is often the direct result of magma forcing its way up toward the surface. 3 What is Volcanic Tremor Ø Volcanic tremor, a type of continuous, rhythmic ground shaking different from the discrete sharp jolts characteristic of earthquakes. Ø Such continuous ground vibrations, commonly associated with eruptions, are interpreted to reflect subsurface movement of fluids, either gas or magma. 4 What is Volcanic Tremor Harmonic tremor signal recorded at Semeru, Indonesia. Up to six overtones can be recognized starting with a fundamental mode located at roughly 0.8 Hz. 5 Methodology; why music processing tools? Ø Large number of data Ø Urgent need to develop new strategies to: Identify and extract data Reduction size strategies Classify records according to their origins Ø Also still there are many unsolved questions about mechanism of generation of different signals in the earth Using the similarity of seismic and acoustic waveforms 6 Methodology; from geophysics to music domain Transfer Geophysical Using New data into Data music processing musical (volcanic analysi method in format tremor) s tools seismology (Wav) Develop innovative seismological data processing methods by borrowing from the expertise developed in the field of MIR. -
Cambridge University Press 978-1-108-44568-9 — Active Faults of the World Robert Yeats Index More Information
Cambridge University Press 978-1-108-44568-9 — Active Faults of the World Robert Yeats Index More Information Index Abancay Deflection, 201, 204–206, 223 Allmendinger, R. W., 206 Abant, Turkey, earthquake of 1957 Ms 7.0, 286 allochthonous terranes, 26 Abdrakhmatov, K. Y., 381, 383 Alpine fault, New Zealand, 482, 486, 489–490, 493 Abercrombie, R. E., 461, 464 Alps, 245, 249 Abers, G. A., 475–477 Alquist-Priolo Act, California, 75 Abidin, H. Z., 464 Altay Range, 384–387 Abiz, Iran, fault, 318 Alteriis, G., 251 Acambay graben, Mexico, 182 Altiplano Plateau, 190, 191, 200, 204, 205, 222 Acambay, Mexico, earthquake of 1912 Ms 6.7, 181 Altunel, E., 305, 322 Accra, Ghana, earthquake of 1939 M 6.4, 235 Altyn Tagh fault, 336, 355, 358, 360, 362, 364–366, accreted terrane, 3 378 Acocella, V., 234 Alvarado, P., 210, 214 active fault front, 408 Álvarez-Marrón, J. M., 219 Adamek, S., 170 Amaziahu, Dead Sea, fault, 297 Adams, J., 52, 66, 71–73, 87, 494 Ambraseys, N. N., 226, 229–231, 234, 259, 264, 275, Adria, 249, 250 277, 286, 288–290, 292, 296, 300, 301, 311, 321, Afar Triangle and triple junction, 226, 227, 231–233, 328, 334, 339, 341, 352, 353 237 Ammon, C. J., 464 Afghan (Helmand) block, 318 Amuri, New Zealand, earthquake of 1888 Mw 7–7.3, 486 Agadir, Morocco, earthquake of 1960 Ms 5.9, 243 Amurian Plate, 389, 399 Age of Enlightenment, 239 Anatolia Plate, 263, 268, 292, 293 Agua Blanca fault, Baja California, 107 Ancash, Peru, earthquake of 1946 M 6.3 to 6.9, 201 Aguilera, J., vii, 79, 138, 189 Ancón fault, Venezuela, 166 Airy, G. -
Seismic Wave Triggering of Nonvolcanic Tremor, Episodic Tremor and Slip, and Earthquakes on Vancouver Island Justin L
JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 114, B00A01, doi:10.1029/2008JB005875, 2009 Click Here for Full Article Seismic wave triggering of nonvolcanic tremor, episodic tremor and slip, and earthquakes on Vancouver Island Justin L. Rubinstein,1,2 Joan Gomberg,3 John E. Vidale,1 Aaron G. Wech,1 Honn Kao,4 Kenneth C. Creager,1 and Garry Rogers4 Received 16 June 2008; revised 14 October 2008; accepted 20 November 2008; published 19 February 2009. [1] We explore the physical conditions that enable triggering of nonvolcanic tremor and earthquakes by considering local seismic activity on Vancouver Island, British Columbia during and immediately after the arrival of large-amplitude seismic waves from 30 teleseismic and 17 regional or local earthquakes. We identify tremor triggered by four of the teleseismic earthquakes. The close temporal and spatial proximity of triggered tremor to ambient tremor and aseismic slip indicates that when a fault is close to or undergoing failure, it is particularly susceptible to triggering of further events. The amplitude of the triggering waves also influences the likelihood of triggering both tremor and earthquakes such that large amplitude waves triggered tremor in the absence of detectable aseismic slip or ambient tremor. Tremor and energy radiated from regional/local earthquakes share the same frequency passband so that tremor cannot be identified during these smaller, more frequent events. We confidently identify triggered local earthquakes following only one teleseism, that with the largest amplitude, and four regional or local events that generated vigorous aftershock sequences in their immediate vicinity. Earthquakes tend to be triggered in regions different from tremor and with high ambient seismicity rates. -
Brief Communication: the Role of Geophysical Imaging in Local Landslide Early Warning Systems
https://doi.org/10.5194/nhess-2021-225 Preprint. Discussion started: 29 July 2021 c Author(s) 2021. CC BY 4.0 License. Brief communication: The role of geophysical imaging in local landslide early warning systems 1 2 1 3 1 Jim S. Whiteley , , Arnaud Watlet , J. Michael Kendall , Jonathan E. Chambers 1Shallow Geohazards and Earth Observation, British Geological Survey, Environmental Science Centre, Nicker Hill, 5 Nottingham, NG12 5GG, United Kingdom. 2School of Earth Sciences, University of Bristol, Wills Memorial Building, Queens Road, Bristol, BS8 1RJ, United Kingdom. 3University of Oxford, Department of Earth Sciences, South Parks Road, Oxford, OX1 3AN, United Kingdom Correspondence to: J.S. Whiteley ([email protected]) Abstract. We summarise the contribution of geophysical imaging to local landslide early warning systems (LoLEWS), 10 highlighting how LoLEWS design and monitoring components benefit from the enhanced spatial and temporal resolutions of time-lapse geophysical imaging. In addition, we discuss how with appropriate laboratory-based petrophysical transforms, these geophysical data can be crucial for future slope failure forecasting and modelling, linking other methods of remote sensing and intrusive monitoring across different scales. We conclude that in light of ever increasing spatiotemporal resolutions of data acquisition, geophysical monitoring should be a more widely considered technology in the toolbox of methods available to 15 stakeholders operating LoLEWS. 1 Introduction Landslide mitigation measures are broadly divided in to two types: engineering approaches to reduce frequency or intensity of failures; and vulnerability reduction measures that de-risk exposed elements (Pecoraro et al., 2019). Here we concentrate on the latter, through the use of landslide early warning systems (LEWS). -
Geophysical Imaging of Permafrost in the SW Svalbard – the Result of Two High Arctic Expeditions to Spitsbergen
EGU2020-8136, updated on 25 Sep 2021 https://doi.org/10.5194/egusphere-egu2020-8136 EGU General Assembly 2020 © Author(s) 2021. This work is distributed under the Creative Commons Attribution 4.0 License. Geophysical imaging of permafrost in the SW Svalbard – the result of two high arctic expeditions to Spitsbergen Mariusz Majdanski1, Artur Marciniak1, Bartosz Owoc1, Wojciech Dobiński2, Tomasz Wawrzyniak1, Marzena Osuch1, Adam Nawrot1, and Michał Glazer2 1Institute of Geophysics, Polish Academy of Sciences, Warsaw, Poland ([email protected]) 2Department of Earth Sciences, University of Silesia, Sosnowiec, Poland The Arctic regions are the place of the fastest observed climate change. One of the indicators of such evolution are changes occurring in the glaciers and the subsurface in the permafrost. The active layer of the permafrost as the shallowest one is well measured by multiple geophysical techniques and in-situ measurements. Two high arctic expeditions have been organized to use seismic methods to recognize the shape of the permafrost in two seasons: with the unfrozen ground (October 2017) and frozen ground (April 2018). Two seismic profiles have been designed to visualize the shape of permafrost between the sea coast and the slope of the mountain, and at the front of a retreating glacier. For measurements, a stand-alone seismic stations has been used with accelerated weight drop with in- house modifications and timing system. Seismic profiles were acquired in a time-lapse manner and were supported with GPR and ERT measurements, and continuous temperature monitoring in shallow boreholes. Joint interpretation of seismic and auxiliary data using Multichannel analysis of surface waves, First arrival travel-time tomography and Reflection imaging show clear seasonal changes affecting the active layer where P-wave velocities are changing from 3500 to 5200 m/s. -
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. -
Summary of the New W4300 Course in DEES: “The Earth's Deep Interior” Instructor: Paul G
Summary of the new W4300 course in DEES: “The Earth's Deep Interior” Instructor: Paul G. Richards ([email protected]) This course emphasizes the geophysical study of Earth structure below the crust, drawing upon geodesy, geomagnetism, gravity, thermal studies, seismology, and some geochemistry. It covers the principal techniques by which discoveries have been made in deep Earth structure, and describes particular features of the mantle, and fluid and solid cores, such as: • the upper mantle beneath old and young oceans and continents • the transition zone in the mantle between about 400 and 700 km depth (within which density and elastic moduli increase anomalously with depth), • the lowermost mantle and core/mantle boundary (across which density doubles and sound speed halves), and • the outer core/inner core boundary (discovered by seismology, and profoundly affecting the Earth's magnetic field). The course is part of the core curriculum for graduate students in solid Earth geophysics and marine geophysics, is an elective for solid Earth geochemistry and geology, and is accessible to undergraduate science majors with adequate math and physics. The course, together with EESC W 4950x (Math Methods in the Earth Sciences), replaces the previous W 4945x – 4946y (Geophysical Theory I and II). It includes parts of previous courses (no longer listed) in seismology, geomagnetism, and thermal history. Emphasis is on current structure, rather than evaluation of dynamic processes (such as convection). Prerequisites calculus, differential -
Seismic Wavefield Imaging of Earth's Interior Across Scales
TECHNICAL REVIEWS Seismic wavefield imaging of Earth’s interior across scales Jeroen Tromp Abstract | Seismic full- waveform inversion (FWI) for imaging Earth’s interior was introduced in the late 1970s. Its ultimate goal is to use all of the information in a seismogram to understand the structure and dynamics of Earth, such as hydrocarbon reservoirs, the nature of hotspots and the forces behind plate motions and earthquakes. Thanks to developments in high- performance computing and advances in modern numerical methods in the past 10 years, 3D FWI has become feasible for a wide range of applications and is currently used across nine orders of magnitude in frequency and wavelength. A typical FWI workflow includes selecting seismic sources and a starting model, conducting forward simulations, calculating and evaluating the misfit, and optimizing the simulated model until the observed and modelled seismograms converge on a single model. This method has revealed Pleistocene ice scrapes beneath a gas cloud in the Valhall oil field, overthrusted Iberian crust in the western Pyrenees mountains, deep slabs in subduction zones throughout the world and the shape of the African superplume. The increased use of multi- parameter inversions, improved computational and algorithmic efficiency , and the inclusion of Bayesian statistics in the optimization process all stand to substantially improve FWI, overcoming current computational or data- quality constraints. In this Technical Review, FWI methods and applications in controlled- source and earthquake seismology are discussed, followed by a perspective on the future of FWI, which will ultimately result in increased insight into the physics and chemistry of Earth’s interior. -
Hawaiian Volcanoes: from Source to Surface Site Waikolao, Hawaii 20 - 24 August 2012
AGU Chapman Conference on Hawaiian Volcanoes: From Source to Surface Site Waikolao, Hawaii 20 - 24 August 2012 Conveners Michael Poland, USGS – Hawaiian Volcano Observatory, USA Paul Okubo, USGS – Hawaiian Volcano Observatory, USA Ken Hon, University of Hawai'i at Hilo, USA Program Committee Rebecca Carey, University of California, Berkeley, USA Simon Carn, Michigan Technological University, USA Valerie Cayol, Obs. de Physique du Globe de Clermont-Ferrand Helge Gonnermann, Rice University, USA Scott Rowland, SOEST, University of Hawai'i at M noa, USA Financial Support 2 AGU Chapman Conference on Hawaiian Volcanoes: From Source to Surface Site Meeting At A Glance Sunday, 19 August 2012 1600h – 1700h Welcome Reception 1700h – 1800h Introduction and Highlights of Kilauea’s Recent Eruption Activity Monday, 20 August 2012 0830h – 0900h Welcome and Logistics 0900h – 0945h Introduction – Hawaiian Volcano Observatory: Its First 100 Years of Advancing Volcanism 0945h – 1215h Magma Origin and Ascent I 1030h – 1045h Coffee Break 1215h – 1330h Lunch on Your Own 1330h – 1430h Magma Origin and Ascent II 1430h – 1445h Coffee Break 1445h – 1600h Magma Origin and Ascent Breakout Sessions I, II, III, IV, and V 1600h – 1645h Magma Origin and Ascent III 1645h – 1900h Poster Session Tuesday, 21 August 2012 0900h – 1215h Magma Storage and Island Evolution I 1215h – 1330h Lunch on Your Own 1330h – 1445h Magma Storage and Island Evolution II 1445h – 1600h Magma Storage and Island Evolution Breakout Sessions I, II, III, IV, and V 1600h – 1645h Magma Storage -
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. -
The Central Asia Collision Zone: Numerical Modelling of the Lithospheric Structure and the Present-Day Kinematics
Th e Central Asia collision zone: numerical modelling of the lithospheric structure and the present - day kinematics Lavinia Tunini A questa tesi doctoral està subjecta a l a llicència Reconeixement - NoComercial – SenseObraDerivada 3.0. Espanya de Creative Commons . Esta tesis doctoral está sujeta a la licencia Reconocimiento - NoComercial – SinObraDerivada 3.0. España de Creative Commons . Th is doctoral thesis is license d under the Creative Commons Attribution - NonCommercial - NoDerivs 3.0. Spain License . The Central Asia collision zone: numerical modelling of the lithospheric structure and the present-day kinematics Ph.D. thesis presented at the Faculty of Geology of the University of Barcelona to obtain the Degree of Doctor in Earth Sciences Ph.D. student: Lavinia Tunini 1 Supervisors: Tutor: Dra. Ivone Jiménez-Munt 1 Prof. Dr. Juan José Ledo Fernández 2 Prof. Dr. Manel Fernàndez Ortiga 1 1 Institute of Earth Sciences Jaume Almera 2 Department of Geodynamics and Geophysics of the University of Barcelona This thesis has been prepared at the Institute of Earth Sciences Jaume Almera Consejo Superior de Investigaciones Científicas (CSIC) March 2015 Alla mia famiglia La natura non ha fretta, eppure tutto si realizza. – Lao Tzu Agradecimientos En mano tenéis un trabajo de casi 4 años, 173 páginas que no hubieran podido salir a luz sin el apoyo de quienes me han ayudado durante este camino, permitiendo acabar la Tesis antes que la Tesis acabase conmigo. En primer lugar quiero agradecer mis directores de tesis, Ivone Jiménez-Munt y Manel Fernàndez. Gracias por haberme dado la oportunidad de entrar en el proyecto ATIZA, de aprender de la modelización numérica, de participar a múltiples congresos y presentaciones, y, mientras, compartir unas cervezas.