Procedures for Estimating Earthquake Ground Motions
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Processing of Strong-Motion Accelerograms: Needs, Options and Consequences
Soil Dynamics and Earthquake Engineering 25 (2005) 93–115 www.elsevier.com/locate/soildyn Processing of strong-motion accelerograms: needs, options and consequences David M. Boorea, Julian J. Bommerb,* aUS Geological Survey, 345 Middlefield Road, Menlo Park, CA 94025, USA bCivil and Environmental Engineering, Imperial College London, London SW7 2AZ, UK Accepted 25 October 2004 Abstract Recordings from strong-motion accelerographs are of fundamental importance in earthquake engineering, forming the basis for all characterizations of ground shaking employed for seismic design. The recordings, particularly those from analog instruments, invariably contain noise that can mask and distort the ground-motion signal at both high and low frequencies. For any application of recorded accelerograms in engineering seismology or earthquake engineering, it is important to identify the presence of this noise in the digitized time- history and its influence on the parameters that are to be derived from the records. If the parameters of interest are affected by noise then appropriate processing needs to be applied to the records, although it must be accepted from the outset that it is generally not possible to recover the actual ground motion over a wide range of frequencies. There are many schemes available for processing strong-motion data and it is important to be aware of the merits and pitfalls associated with each option. Equally important is to appreciate the effects of the procedures on the records in order to avoid errors in the interpretation and use of the results. Options for processing strong-motion accelerograms are presented, discussed and evaluated from the perspective of engineering application. -
Guideline for Extraction of Ground Motion Parameters for Scientific Hydraulic Fracturing Review Panel
Guideline for Extraction of Ground Motion Parameters for Scientific Hydraulic Fracturing Review Panel Alireza Babaie Mahani Ph.D. P.Geo. Mahan Geophysical Consulting Inc. Victoria, BC Email: [email protected] Website: www.mahangeo.com Executive Summary The Scientific Review of Hydraulic Fracturing in British Columbia (2019) provides the key findings of a scientific panel on the topic of hydraulic fracturing in British Columbia and the associated environmental risks. As indicated in the report, the panel recommends preparation of guidelines for standard calculation of earthquake magnitude and ground motion parameters. Since Babaie Mahani and Kao (2019 and 2020) have addressed the methodology for calculation of local magnitude in two publications, this report deals with standard methodologies for extraction of ground motion parameters from recorded earthquake waveforms. The guidelines include data from both types of seismic sensors that are used for induced seismicity monitoring; seismometers that record ground motion velocities and accelerometers that are designed to record strong ground accelerations at short distances. Waveforms from the November 30, 2018 induced earthquake with moment magnitude (Mw) of 4.6 that occurred in northeast British Columbia within the Montney unconventional resource play are presented for better understanding of the processing steps. Data Formats The standard format that is used to archive earthquake data is called the SEED format (Standard for the Exchange of Earthquake Data; https://ds.iris.edu/ds/nodes/dmc/data/formats/seed/). When both the time series data and metadata are archived in one file, the name full-SEED is also used. miniSEED is the stripped down version of SEED that only includes waveform data (https://ds.iris.edu/ds/nodes/dmc/data/formats/miniseed/). -
Seismic Acceleration and Displacement Demand Profiles of Non-Structural Elements in Hospital Buildings
buildings Article Seismic Acceleration and Displacement Demand Profiles of Non-Structural Elements in Hospital Buildings Giammaria Gabbianelli 1 , Daniele Perrone 1,2,* , Emanuele Brunesi 3 and Ricardo Monteiro 1 1 University School for Advanced Studies IUSS Pavia, 27100 Pavia, Italy; [email protected] (G.G.); [email protected] (R.M.) 2 Department of Engineering for Innovation, University of Salento, 73100 Lecce, Italy 3 European Centre for Training and Research in Earthquake Engineering (EUCENTRE), 27100 Pavia, Italy; [email protected] * Correspondence: [email protected] Received: 23 October 2020; Accepted: 11 December 2020; Published: 15 December 2020 Abstract: The importance of non-structural elements in performance-based seismic design of buildings is presently widely recognized. These elements may significantly affect the functionality of buildings even for low seismic intensities, in particular for the case of critical facilities, such as hospital buildings. One of the most important issues to deal with in the seismic performance assessment of non-structural elements is the definition of the seismic demand. This paper investigates the seismic demand to which the non-structural elements of a case-study hospital building located in a medium–high seismicity region in Italy, are prone. The seismic demand is evaluated for two seismic intensities that correspond to the definition of serviceability limit states, according to Italian and European design and assessment guidelines. Peak floor accelerations, interstorey drifts, absolute acceleration, and relative displacement floor response spectra are estimated through nonlinear time–history analyses. The absolute acceleration floor response spectra are then compared with those obtained from simplified code formulations, highlighting the main shortcomings surrounding the practical application of performance-based seismic design of non-structural elements. -
Rood Et Al 2011 EPSL SNFFZ.Pdf
This article appeared in a journal published by Elsevier. The attached copy is furnished to the author for internal non-commercial research and education use, including for instruction at the authors institution and sharing with colleagues. Other uses, including reproduction and distribution, or selling or licensing copies, or posting to personal, institutional or third party websites are prohibited. In most cases authors are permitted to post their version of the article (e.g. in Word or Tex form) to their personal website or institutional repository. Authors requiring further information regarding Elsevier’s archiving and manuscript policies are encouraged to visit: http://www.elsevier.com/copyright Author's personal copy Earth and Planetary Science Letters 301 (2011) 457–468 Contents lists available at ScienceDirect Earth and Planetary Science Letters journal homepage: www.elsevier.com/locate/epsl Spatiotemporal patterns of fault slip rates across the Central Sierra Nevada frontal fault zone Dylan H. Rood a,b,⁎, Douglas W. Burbank a, Robert C. Finkel c,d a Department of Earth Science, University of California, Santa Barbara, CA 93106, USA b Center for Accelerator Mass Spectrometry, Lawrence Livermore National Laboratory, Livermore, CA 94550, USA c CEREGE, Aix en Provence, France d Department of Earth and Planetary Science, University of California, Berkeley, CA 94720, USA article info abstract Article history: Patterns in fault slip rates through time and space are examined across the transition from the Sierra Nevada Received 23 June 2010 to the Eastern California Shear Zone–Walker Lane belt. At each of four sites along the eastern Sierra Nevada Received in revised form 30 October 2010 frontal fault zone between 38 and 39° N latitude, geomorphic markers, such as glacial moraines and outwash Accepted 2 November 2010 terraces, are displaced by a suite of range-front normal faults. -
Department D'analyse De Surete
COMMISSARIAT A LENERGIE ATOMIQUE XA04NO298 INSTITUT DE PROTECTION ET DE SURETE NUCLEAIRE DEPARTMENT D'ANALYSE DE SURETE INIS-XA-N--027 RAPPORT DAS/733 MAIN FACTORS AECTING STRONG GROUND MOTION CALCULATIONS CRITICAL REVIEW AND ASESSMENT. MOHAMMADIOUN B. PECKER A. RAPPORT DAS/733 MAIN FACTORS AECTING STRONG GROUND MOTION CALCULATIONS CRITICAL REVIEW AND ASSESSMENT. MOHAMMADIOUN B. , PECKER A. 1990 * DAS/SASC ** Soci6t6 G6odynamique et Structure I I MAIN FACTORS AFFECTING STRONG GROUND MOTION CALCULATIONS: CRITICAL REVIEW AND ASSESSMENT BAGHER MOHAMMADIOUN * AND ALUN PECKER" 1. 1. INTRODUCTION in the interests of guarding lives and property against the effects of earthquakes, building codes are frequently enforced when recting conventional structures, usually calling for simple, static calculations. Where more vulnerable facilities are involved, the failure of which, or of parts of which, could subject the environment to harmful substances, more sophisticated methods are used to compute or verify their design, often accompanied by safety margins intended to compen- sate for uncertainties encountered at various stages of the analysis that begins with input seismic data and culminates with an effective anti-seismic dsign. The forthcoming discussion will deal with what is known of the characteristics of strong ground motion, highly variable according to contM without entering into the problems raised by scismotectonic studies, which actually constitute the first aspect that must be addressed when performing such an analysis. Our conclusion will be devoted to cogent R & D work in this area. 1.2. STRONG MOTION DATA The earliest record obtained with a strong motion accelerograph dates back to 1933 and was triggered by the Long Beach, California earthquake. -
Position, Displacement, Velocity Big Picture
Position, Displacement, Velocity Big Picture I Want to know how/why things move I Need a way to describe motion mathematically: \Kinematics" I Tools of kinematics: calculus (rates) and vectors (directions) I Chapters 2, 4 are all about kinematics I First 1D, then 2D/3D I Main ideas: position, velocity, acceleration Language is crucial Physics uses ordinary words but assigns specific technical meanings! WORD ORDINARY USE PHYSICS USE position where something is where something is velocity speed speed and direction speed speed magnitude of velocity vec- tor displacement being moved difference in position \as the crow flies” from one instant to another Language, continued WORD ORDINARY USE PHYSICS USE total distance displacement or path length traveled path length trav- eled average velocity | displacement divided by time interval average speed total distance di- total distance divided by vided by time inter- time interval val How about some examples? Finer points I \instantaneous" velocity v(t) changes from instant to instant I graphically, it's a point on a v(t) curve or the slope of an x(t) curve I average velocity ~vavg is not a function of time I it's defined for an interval between instants (t1 ! t2, ti ! tf , t0 ! t, etc.) I graphically, it's the \rise over run" between two points on an x(t) curve I in 1D, vx can be called v I it's a component that is positive or negative I vectors don't have signs but their components do What you need to be able to do I Given starting/ending position, time, speed for one or more trip legs, calculate average -
Prediction of Spectral Acceleration Response Ordinates Based on PGA Attenuation
Prediction of Spectral Acceleration Response Ordinates Based on PGA Attenuation a),c) b),c) Vladimir Graizer, M.EERI, and Erol Kalkan, M.EERI Developed herein is a new peak ground acceleration (PGA)-based predictive model for 5% damped pseudospectral acceleration (SA) ordinates of free-field horizontal component of ground motion from shallow-crustal earthquakes. The predictive model of ground motion spectral shape (i.e., normalized spectrum) is generated as a continuous function of few parameters. The proposed model eliminates the classical exhausted matrix of estimator coefficients, and provides significant ease in its implementation. It is structured on the Next Generation Attenuation (NGA) database with a number of additions from recent Californian events including 2003 San Simeon and 2004 Parkfield earthquakes. A unique feature of the model is its new functional form explicitly integrating PGA as a scaling factor. The spectral shape model is parameterized within an approximation function using moment magnitude, closest distance to the fault (fault distance) and VS30 (average shear-wave velocity in the upper 30 m) as independent variables. Mean values of its estimator coefficients were computed by fitting an approximation function to spectral shape of each record using robust nonlinear optimization. Proposed spectral shape model is independent of the PGA attenuation, allowing utilization of various PGA attenuation relations to estimate the response spectrum of earthquake recordings. ͓DOI: 10.1193/1.3043904͔ INTRODUCTION Since it was first introduced by Biot (1933) and later conveyed to engineering appli- cations by Housner (1959) and Newmark et al. (1973), the ground motion response spectrum has often been utilized for purposes of recognizing the significant characteris- tics of accelerograms and evaluating the response of structures to earthquake ground shaking. -
A Review of the Seismic Hazard Zonation in National Building Codes in the Context of Eurocode 8
A REVIEW OF THE SEISMIC HAZARD ZONATION IN NATIONAL BUILDING CODES IN THE CONTEXT OF EUROCODE 8 Support to the implementation, harmonization and further development of the Eurocodes G. Solomos, A. Pinto, S. Dimova EUR 23563 EN - 2008 A REVIEW OF THE SEISMIC HAZARD ZONATION IN NATIONAL BUILDING CODES IN THE CONTEXT OF EUROCODE 8 Support to the implementation, harmonization and further development of the Eurocodes G. Solomos, A. Pinto, S. Dimova EUR 23563 EN - 2008 The mission of the JRC is to provide customer-driven scientific and technical support for the conception, development, implementation and monitoring of EU policies. As a service of the European Commission, the JRC functions as a reference centre of science and technology for the Union. Close to the policy-making process, it serves the common interest of the Member States, while being independent of special interests, whether private or national. European Commission Joint Research Centre Contact information Address: JRC, ELSA Unit, TP 480, I-21020, Ispra(VA), Italy E-mail: [email protected] Tel.: +39-0332-789989 Fax: +39-0332-789049 http://www.jrc.ec.europa.eu Legal Notice Neither the European Commission nor any person acting on behalf of the Commission is responsible for the use which might be made of this publication. A great deal of additional information on the European Union is available on the Internet. It can be accessed through the Europa server http://europa.eu/ JRC 48352 EUR 23563 EN ISSN 1018-5593 Luxembourg: Office for Official Publications of the European Communities © European Communities, 2008 Reproduction is authorised provided the source is acknowledged Printed in Italy Executive Summary The Eurocodes are envisaged to form the basis for structural design in the European Union and they should enable engineering services to be used across borders for the design of construction works. -
U. S. Department of the Interior U. S. Geological Survey
U. S. DEPARTMENT OF THE INTERIOR U. S. GEOLOGICAL SURVEY RELATION OF ARIAS INTENSITY TO MAGNITUDE AND DISTANCE IN CALIFORNIA by Raymond C. Wilson1 OPEN-FILE REPORT 93-556 This report is preliminary and has not been reviewed for conformity with U.S. Geological Survey editorial standards or with the North American Stratigraphic Code. Any use of trade, product, or firm names is for descriptive purposes only and does not imply endorsement by the U. S.. Government. iMenlo Park, California 94025 September 1993 TABLE OF CONTENTS Abstract..................................................................................! Introduction............................................................................! Definition of Arias Intensity......................................................3 Relating Intensity to the Seismic Source.....................................4 Arias Intensity and the Seismic Source Parameters................4 Arias Intensity as a Function of Moment Magnitude...............6 Empirical Tests of the Theoretical M/R/Ia Model..........................6 Arias Intensity as a Function of Distance...............................8 Arias Intensity as a Function of Magnitude.......................... 12 Analysis of Residuals from a Combined Data Set................... 14 A Possible Simplification.................................................... 18 Summary of Empirical Analyses......................................... 18 Modifications of the M/R/Ia Relation for Special Conditions ........ 20 Site-Response Effects......................................................... -
Abdus Salam United Nations Educational, Scientific and Cultural Organization International Centre XA0100122
the IC/2000/170 abdus salam united nations educational, scientific and cultural organization international centre XA0100122 international atomic energy agency for theoretical physics SHAPE ANALYSIS OF ISOSEISMALS BASED ON EMPIRICAL AND SYNTHETIC DATA G. Molchan T. Kronrod and G.F. Panza SEgi 'A*'.' Sri 32/ 05 • _ ^BH |« # ,-a?; IC/2000/170 United Nations Educational Scientific and Cultural Organization and International Atomic Energy Agency THE ABDUS SALAM INTERNATIONAL CENTRE FOR THEORETICAL PHYSICS SHAPE ANALYSIS OF ISOSEISMALS BASED ON EMPIRICAL AND SYNTHETIC DATA G. Molchan1, T. Kronrod, International Institute of Earthquake Prediction Theory and Mathematical Geophysics, Russian Academy of Sciences, Warshavskoe sh., 79, k.2, Moscow 113556, Russian Federation and The Abdus Salam International Centre for Theoretical Physics, SAND Group, Trieste, Italy, and G.F. Panza Department of Earth Sciences, University of Trieste, Trieste, Italy and The Abdus Salam International Centre for Theoretical Physics, SAND Group, Trieste, Italy. MIRAMARE - TRIESTE November 2000 'E-mail: [email protected]; Tel. +007 (095) 110-7795; Fax: +007 (095) 310-7032 Abstract. We present an attempt to compare modeled ground motion acceleration fields with macroseismic observations. Two techniques for the representation of the observed intensities by isoseismals, a smoothing technique and one which visualizes the local uncertainty of an isoseis- mal, are tested with synthetic and observed data. We show how noise in the data and irregulari- ties in the distribution of observation sites affect the resolution of the isoseismal's shape. In ad- dition to "standard" elongated shapes, we identify cross-like patterns in the macroseismic obser- vations for two Italian earthquakes of strike-slip type; similar patterns are displayed by the theo- retical peak acceleration fields calculated assuming the point source models given in the litera- ture. -
Chapter 3 Motion in Two and Three Dimensions
Chapter 3 Motion in Two and Three Dimensions 3.1 The Important Stuff 3.1.1 Position In three dimensions, the location of a particle is specified by its location vector, r: r = xi + yj + zk (3.1) If during a time interval ∆t the position vector of the particle changes from r1 to r2, the displacement ∆r for that time interval is ∆r = r1 − r2 (3.2) = (x2 − x1)i +(y2 − y1)j +(z2 − z1)k (3.3) 3.1.2 Velocity If a particle moves through a displacement ∆r in a time interval ∆t then its average velocity for that interval is ∆r ∆x ∆y ∆z v = = i + j + k (3.4) ∆t ∆t ∆t ∆t As before, a more interesting quantity is the instantaneous velocity v, which is the limit of the average velocity when we shrink the time interval ∆t to zero. It is the time derivative of the position vector r: dr v = (3.5) dt d = (xi + yj + zk) (3.6) dt dx dy dz = i + j + k (3.7) dt dt dt can be written: v = vxi + vyj + vzk (3.8) 51 52 CHAPTER 3. MOTION IN TWO AND THREE DIMENSIONS where dx dy dz v = v = v = (3.9) x dt y dt z dt The instantaneous velocity v of a particle is always tangent to the path of the particle. 3.1.3 Acceleration If a particle’s velocity changes by ∆v in a time period ∆t, the average acceleration a for that period is ∆v ∆v ∆v ∆v a = = x i + y j + z k (3.10) ∆t ∆t ∆t ∆t but a much more interesting quantity is the result of shrinking the period ∆t to zero, which gives us the instantaneous acceleration, a. -
Rotational Motion of Electric Machines
Rotational Motion of Electric Machines • An electric machine rotates about a fixed axis, called the shaft, so its rotation is restricted to one angular dimension. • Relative to a given end of the machine’s shaft, the direction of counterclockwise (CCW) rotation is often assumed to be positive. • Therefore, for rotation about a fixed shaft, all the concepts are scalars. 17 Angular Position, Velocity and Acceleration • Angular position – The angle at which an object is oriented, measured from some arbitrary reference point – Unit: rad or deg – Analogy of the linear concept • Angular acceleration =d/dt of distance along a line. – The rate of change in angular • Angular velocity =d/dt velocity with respect to time – The rate of change in angular – Unit: rad/s2 position with respect to time • and >0 if the rotation is CCW – Unit: rad/s or r/min (revolutions • >0 if the absolute angular per minute or rpm for short) velocity is increasing in the CCW – Analogy of the concept of direction or decreasing in the velocity on a straight line. CW direction 18 Moment of Inertia (or Inertia) • Inertia depends on the mass and shape of the object (unit: kgm2) • A complex shape can be broken up into 2 or more of simple shapes Definition Two useful formulas mL2 m J J() RRRR22 12 3 1212 m 22 JRR()12 2 19 Torque and Change in Speed • Torque is equal to the product of the force and the perpendicular distance between the axis of rotation and the point of application of the force. T=Fr (Nm) T=0 T T=Fr • Newton’s Law of Rotation: Describes the relationship between the total torque applied to an object and its resulting angular acceleration.