Title Glossary of Interest to Earthquake and Engineering Seismologists
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Glossary Physics (I-Introduction)
1 Glossary Physics (I-introduction) - Efficiency: The percent of the work put into a machine that is converted into useful work output; = work done / energy used [-]. = eta In machines: The work output of any machine cannot exceed the work input (<=100%); in an ideal machine, where no energy is transformed into heat: work(input) = work(output), =100%. Energy: The property of a system that enables it to do work. Conservation o. E.: Energy cannot be created or destroyed; it may be transformed from one form into another, but the total amount of energy never changes. Equilibrium: The state of an object when not acted upon by a net force or net torque; an object in equilibrium may be at rest or moving at uniform velocity - not accelerating. Mechanical E.: The state of an object or system of objects for which any impressed forces cancels to zero and no acceleration occurs. Dynamic E.: Object is moving without experiencing acceleration. Static E.: Object is at rest.F Force: The influence that can cause an object to be accelerated or retarded; is always in the direction of the net force, hence a vector quantity; the four elementary forces are: Electromagnetic F.: Is an attraction or repulsion G, gravit. const.6.672E-11[Nm2/kg2] between electric charges: d, distance [m] 2 2 2 2 F = 1/(40) (q1q2/d ) [(CC/m )(Nm /C )] = [N] m,M, mass [kg] Gravitational F.: Is a mutual attraction between all masses: q, charge [As] [C] 2 2 2 2 F = GmM/d [Nm /kg kg 1/m ] = [N] 0, dielectric constant Strong F.: (nuclear force) Acts within the nuclei of atoms: 8.854E-12 [C2/Nm2] [F/m] 2 2 2 2 2 F = 1/(40) (e /d ) [(CC/m )(Nm /C )] = [N] , 3.14 [-] Weak F.: Manifests itself in special reactions among elementary e, 1.60210 E-19 [As] [C] particles, such as the reaction that occur in radioactive decay. -
Oscillating Currents
Oscillating Currents • Ch.30: Induced E Fields: Faraday’s Law • Ch.30: RL Circuits • Ch.31: Oscillations and AC Circuits Review: Inductance • If the current through a coil of wire changes, there is an induced emf proportional to the rate of change of the current. •Define the proportionality constant to be the inductance L : di εεε === −−−L dt • SI unit of inductance is the henry (H). LC Circuit Oscillations Suppose we try to discharge a capacitor, using an inductor instead of a resistor: At time t=0 the capacitor has maximum charge and the current is zero. Later, current is increasing and capacitor’s charge is decreasing Oscillations (cont’d) What happens when q=0? Does I=0 also? No, because inductor does not allow sudden changes. In fact, q = 0 means i = maximum! So now, charge starts to build up on C again, but in the opposite direction! Textbook Figure 31-1 Energy is moving back and forth between C,L 1 2 1 2 UL === UB === 2 Li UC === UE === 2 q / C Textbook Figure 31-1 Mechanical Analogy • Looks like SHM (Ch. 15) Mass on spring. • Variable q is like x, distortion of spring. • Then i=dq/dt , like v=dx/dt , velocity of mass. By analogy with SHM, we can guess that q === Q cos(ωωω t) dq i === === −−−ωωωQ sin(ωωω t) dt Look at Guessed Solution dq q === Q cos(ωωω t) i === === −−−ωωωQ sin(ωωω t) dt q i Mathematical description of oscillations Note essential terminology: amplitude, phase, frequency, period, angular frequency. You MUST know what these words mean! If necessary review Chapters 10, 15. -
Experiment No. 3 Oscilloscope and Function Generator
Experiment No. 3 Oscilloscope and Function Generator An oscilloscope is a voltmeter that can measure a fast changing wave form. Wave forms A simple wave form is characterized by its period and amplitude. A function generator can generate different wave forms. 1 Part 1 of the experiment (together) Generate a square wave of frequency of 1.8 kHz with the function generator. Measure the amplitude and frequency with the Fluke DMM. Measure the amplitude and frequency with the oscilloscope. 2 The voltage amplitude has 2.4 divisions. Each division means 5.00 V. The amplitude is (5)(2.4) = 12.0 V. The Fluke reading was 11.2 V. The period (T) of the wave has 2.3 divisions. Each division means 250 s. The period is (2.3)(250 s) = 575 s. 1 1 f 1739 Hz The frequency of the wave = T 575 10 6 The Fluke reading was 1783 Hz The error is at least 0.05 divisions. The accuracy can be improved by displaying the wave form bigger. 3 Now, we have two amplitudes = 4.4 divisions. One amplitude = 2.2 divisions. Each division = 5.00 V. One amplitude = 11.0 V Fluke reading was 11.2 V T = 5.7 divisions. Each division = 100 s. T = 570 s. Frequency = 1754 Hz Fluke reading was 1783 Hz. It was always better to get a bigger display. 4 Part 2 of the experiment -Measuring signals from the DVD player. Next turn on the DVD Player and turn on the accessory device that is attached to the top of the DVD player. -
Peak and Root-Mean-Square Accelerations Radiated from Circular Cracks and Stress-Drop Associated with Seismic High-Frequency Radiation
J. Phys. Earth, 31, 225-249, 1983 PEAK AND ROOT-MEAN-SQUARE ACCELERATIONS RADIATED FROM CIRCULAR CRACKS AND STRESS-DROP ASSOCIATED WITH SEISMIC HIGH-FREQUENCY RADIATION Teruo YAMASHITA Earthquake Research Institute, the University of Tokyo, Tokyo, Japan (Received July 25, 1983) We derive an approximate expression for far-field spectral amplitude of acceleration radiated by circular cracks. The crack tip velocity is assumed to make abrupt changes, which can be the sources of high-frequency radiation, during the propagation of crack tip. This crack model will be usable as a source model for the study of high-frequency radiation. The expression for the spectral amplitude of acceleration is obtained in the following way. In the high-frequency range its expression is derived, with the aid of geometrical theory of diffraction, by extending the two-dimensional results. In the low-frequency range it is derived on the assumption that the source can be regarded as a point. Some plausible assumptions are made for its behavior in the intermediate- frequency range. Theoretical expressions for the root-mean-square and peak accelerations are derived by use of the spectral amplitude of acceleration obtained in the above way. Theoretically calculated accelerations are compared with observed ones. The observations are shown to be well explained by our source model if suitable stress-drop and crack tip velocity are assumed. Using Brune's model as an earthquake source model, Hanks and McGuire showed that the seismic ac- celerations are well predicted by a stress-drop which is higher than the statically determined stress-drop. However, their conclusion seems less reliable since Brune's source model cannot be applied to the study of high-frequency radiation. -
"Seismites" (Seilacher 1969; Vittori, Sylos-Labini & Serva 1988), Which Include Faults, Sandblows, Folds and Fissures
Radiocarbon Dating of Paleoseismicity Along an Earthquake Fault in Southern Italy Item Type Article; text Authors Calderoni, Gilberto; Petrone, Vincenzo Citation Calderoni, G., & Petrone, V. (1993). Radiocarbon dating of paleoseismicity along an earthquake fault in southern Italy. Radiocarbon, 35(2), 287-293. DOI 10.1017/S0033822200064961 Publisher Department of Geosciences, The University of Arizona Journal Radiocarbon Rights Copyright © by the Arizona Board of Regents on behalf of the University of Arizona. All rights reserved. Download date 27/09/2021 12:51:50 Item License http://rightsstatements.org/vocab/InC/1.0/ Version Final published version Link to Item http://hdl.handle.net/10150/653403 [RADIOCARBON, VOL. 35, No. 2, 1993, P. 287-293] RADIOCARBON DATING OF PALEOSEISMICITY ALONG AN EARTHQUAKE FAULT IN SOUTHERN ITALY GILBERTO CALDERONI and VINCENZO FETRONE Department of Earth Sciences, University of Rome I "La Sapienza" Piazzale Aldo Moro, 5, 00100 Rome Italy ABSTRACT. On 23 November 1980, a major earthquake (M, = 6.9) struck a large area of the southern Apennines (Campania and Lucania regions, southern Italy). This seismic event, the largest in Italy over the last 80 years, almost completely destroyed 15 villages and caused extensive damage to other towns, including Naples. The quake produced the first well-documented example in Italy of surface dislocation, represented by a fault scarp 38 km long. We undertook a study that included 14C dating of organic materials from layers displaced by paleoseismic events to assess the seismologic hazard for the area. We collected peat and charred wood samples from the walls of two trenches excavated across the 1980 fault at Piano di Pecore di Colliano, Salerno, where the sedimentary suite is faulted and warped by five quakes (including that of 1980). -
Amplitude-Probability Distributions for Atmospheric Radio Noise
S 7. •? ^ I ft* 2. 3 NBS MONOGRAPH 23 Amplitude-Probability Distributions for Atmospheric Radio Noise N v " X \t£ , " o# . .. » U.S. DEPARTMENT OF COMMERCE NATIONAL BUREAU OF STANDARDS THE NATIONAL BUREAU OF STANDARDS Functions and Activities The functions of the National Bureau of Standards are set forth in the Act of Congress, March 3, 1901, as amended by Congress in Public Law 619, 1950. These include the development and maintenance of the national standards of measurement and the provision of means and methods for making measurements consistent with these standards; the determination of physical constants and properties of materials; the development of methods and instruments for testing materials, devices, and structures; advisory services to government agencies on scientific and technical problems; inven- tion and development of devices to serve special needs of the Government; and the development of standard practices, codes, and specifications. The work includes basic and applied research, develop- ment, engineering, instrumentation, testing, evaluation, calibration services, and various consultation and information services. Research projects are also performed for other government agencies when the work relates to and supplements the basic program of the Bureau or when the Bureau's unique competence is required. The scope of activities is suggested by the listing of divisions and sections on the inside of the back cover. Publications The results of the Bureau's work take the form of either actual equipment and devices or pub- -
Amplitude Modulation of the AD9850 Direct Digital Synthesizer by Richard Cushing, Applications Engineer
AN-423 a APPLICATION NOTE ONE TECHNOLOGY WAY • P.O. BOX 9106 • NORWOOD, MASSACHUSETTS 02062-9106 • 617/329-4700 Amplitude Modulation of the AD9850 Direct Digital Synthesizer by Richard Cushing, Applications Engineer This application note will offer a method to voltage con- The voltage at the RSET pin is part of the feedback loop of trol or amplitude modulate the output current of the the (internal) control amplifier and must not be exter- AD9850 DDS using an enhancement mode MOSFET to nally altered. The RSET modification circuit, Figure 2, replace the fixed RSET resistor; and a broadband RF uses Q1 as a variable resistor and R2 as a fixed current transformer to combine the DDS DAC outputs to pro- limit resistor in case Q1 is allowed to turn on too much. duce a symmetrical AM modulation envelope. Modula- C1 inhibits noise when Q1 is operated near cutoff. R1 tion with reasonable linearity is possible at rates lowers the input impedance for additional noise preven- exceeding 50 kHz. The AD9850 DDS output current tion. The input voltage to Q1 required to fully modulate (20 mA maximum) is normally set with a fixed resistor the AD9850 output is approximately 1.5 volts p-p and from the RSET (Pin 12) input to ground. The DAC outputs is dc offset by approximately 2.3 volts, see Figure 4. are unipolar and complementary (180 degrees out of TO RSET DC OR AUDIO phase) of each other. D C1 PIN 12 INPUT Q1 510pF Use of an enhancement mode MOSFET is in keeping G 2N7000* with the single supply concept. -
Bulletin 442 Seismic Effects of Quarry Blasting
UNITED STATES DEPARTMENT OF THE INTERIOR HAROLD L. ICKES, Secretary BUREAU OF MINES R. R. SAYERS, Director Bulletin 442 SEISMIC EFFECTS OF QUARRY BLASTING BY J. R. THOENEN and S. L. WINDES UNITED STATES GOVERNMENT PRINTING OFFICE WASHINGTON : 1942 For sale by the Superintendent of Documents, Washington, D. C. ---- Price 15 cents CONTENTS .Pare Introduction _____________________________________________________ _ 1 Object of bulletin _________________________________________________ _ 1 History of study __________________________________________________ _ 2 Acknowledgments------------------------------------------------- 4 Previous publications _____________________________ -_-_---_------_.- & Preliminary studies of building vibrations ____________________________ _ 7 Summary of 1936 quarry tests ______________________________________ _ g; Path of a vibrating point ______________________________________ _ 9 Speed of seismic wave _________________________________________ _ 10 Amplitude of seismic wave _____________________________________ _ 10 Frequency of seismic wave _____________________________________ _ 10 Duration of seismic wave _______________________________ ----- __ _ 10 Correlation of amplitude, frequency, and duration ________________ _ 11 Correlation of amplitude and distance ___________________________ _ 11 Correlation of amplitude and weight of explosive charge ___________ _ 11 Effect of moisture on amplitude ________________________________ _ 11 Effect of geographic direction on amplitude ______________________ _ 12 Effect -
Amplitude Modulation Transmitter Design
Amplitude LAB Modulation 5 Transmitter Design Introduction The motivation behind this project is to design, implement, and test an Amplitude Modulation (AM) Transmitter. The Transmitter consists of a Balanced Modulator circuit which takes an audio signal stream from a Walkman and mixes it with a sinusoidal signal from a 1MHz oscillator. The resulting output is amplified by an output stage before being transmitted through a wire-antenna. AM Transmitter Floorplan: Design Goals Given the limited timeframe, we are providing you with the individual circuits that you need to design and construct. Fig. 1 shows the floorplan for the AM Transmitter. It consists of a Balanced Modulator which multiplies an audio fre- quency (20Hz to ~15kHz) signal with a 1MHz carrier frequency sinusoidal signal. The Balanced Modulator’s output is amplified by an output stage which drives an antenna (in this experiment, the antenna is just a 3” copper wire). The Balanced Modulator (Fig. 2) is essentially an analog multiplier: its time domain output signal, Vout(t) is linearly related to the product of the time domain input signals V1(t) (called the modulation signal) and V2(t) (called the carrier sig- nal). Its transfer function has the form: V ()t = k ⋅⋅V ()t V ()t out 1 2 The Balanced Modulator uses the principle of the dependence of the BJT’s transconductance, gm, on the emitter current bias. In order to demonstrate the principle, consider the load currents IL1 and IL2. From your knowledge of differ- ential amplifier operation, IL1 V1 I – I = g ⋅ V ≈ -------- ⋅ ------ L1 L2 m in VT 2 Also, the bias current IB in the differential amplifiers can be expressed as: V – 0.7 ≈ 2 IB ------------------ RE 1 Lab : Amplitude Modulation Transmitter Design Antenna Balanced O/P stage Walkman Modulator Amplifier 1MHz Oscillator Figure 1 — Amplitude Modulation Transmitter floorplan. -
EE301 – INTRO to AC and SINUSOIDS Learning Objectives
EE301 – INTRO TO AC AND SINUSOIDS Learning Objectives a. Compare AC and DC voltage and current sources as defined by voltage polarity, current direction and magnitude over time b. Define the basic sinusoidal wave equations and waveforms, and determine amplitude, peak to peak values, phase, period, frequency, and angular velocity c. Determine the instantaneous value of a sinusoidal waveform d. Graph sinusoidal wave equations as a function of time and angular velocity using degrees and radians e. Define effective / root mean squared values f. Define phase shift and determine phase differences between same frequency waveforms Alternating Current (AC) With the exception of short-term capacitor and inductor transients, all voltages and currents we have seen up to this point have been “DC”—i.e., fixed in magnitude. Now we shift our focus to “AC” voltage and current sources. AC sources (usually represented by lowercase e(t) or i(t)) have a sinusoidal waveform. For an AC voltage, for example, the voltage polarity changes every cycle. On the other hand, for an AC current, the current changes direction each cycle with the source voltage. Voltage and Current Conventions When e has a positive value, its actual polarity is the same as the reference polarity. When i has a positive value, its actual direction is the same as the reference arrow. 1 9/14/2016 EE301 – INTRO TO AC AND SINUSOIDS Sinusoids Since our ac waveforms (voltages and currents) are sinusoidal, we need to have a ready familiarity with the equation for a sinusoid. The horizontal scale, referred to as the “time scale” can represent degrees or time. -
Oscilloscope Fundamentals 03W-8605-4 Edu.Qxd 3/31/09 1:55 PM Page 2
03W-8605-4_edu.qxd 3/31/09 1:55 PM Page 1 Oscilloscope Fundamentals 03W-8605-4_edu.qxd 3/31/09 1:55 PM Page 2 Oscilloscope Fundamentals Table of Contents The Systems and Controls of an Oscilloscope .18 - 31 Vertical System and Controls . 19 Introduction . 4 Position and Volts per Division . 19 Signal Integrity . 5 - 6 Input Coupling . 19 Bandwidth Limit . 19 The Significance of Signal Integrity . 5 Bandwidth Enhancement . 20 Why is Signal Integrity a Problem? . 5 Horizontal System and Controls . 20 Viewing the Analog Orgins of Digital Signals . 6 Acquisition Controls . 20 The Oscilloscope . 7 - 11 Acquisition Modes . 20 Types of Acquisition Modes . 21 Understanding Waveforms & Waveform Measurements . .7 Starting and Stopping the Acquisition System . 21 Types of Waves . 8 Sampling . 22 Sine Waves . 9 Sampling Controls . 22 Square and Rectangular Waves . 9 Sampling Methods . 22 Sawtooth and Triangle Waves . 9 Real-time Sampling . 22 Step and Pulse Shapes . 9 Equivalent-time Sampling . 24 Periodic and Non-periodic Signals . 10 Position and Seconds per Division . 26 Synchronous and Asynchronous Signals . 10 Time Base Selections . 26 Complex Waves . 10 Zoom . 26 Eye Patterns . 10 XY Mode . 26 Constellation Diagrams . 11 Z Axis . 26 Waveform Measurements . .11 XYZ Mode . 26 Frequency and Period . .11 Trigger System and Controls . 27 Voltage . 11 Trigger Position . 28 Amplitude . 12 Trigger Level and Slope . 28 Phase . 12 Trigger Sources . 28 Waveform Measurements with Digital Oscilloscopes 12 Trigger Modes . 29 Trigger Coupling . 30 Types of Oscilloscopes . .13 - 17 Digital Oscilloscopes . 13 Trigger Holdoff . 30 Digital Storage Oscilloscopes . 14 Display System and Controls . 30 Digital Phosphor Oscilloscopes . -
A Partial Glossary of Spanish Geological Terms Exclusive of Most Cognates
U.S. DEPARTMENT OF THE INTERIOR U.S. GEOLOGICAL SURVEY A Partial Glossary of Spanish Geological Terms Exclusive of Most Cognates by Keith R. Long Open-File Report 91-0579 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, firm, or product names is for descriptive purposes only and does not imply endorsement by the U.S. Government. 1991 Preface In recent years, almost all countries in Latin America have adopted democratic political systems and liberal economic policies. The resulting favorable investment climate has spurred a new wave of North American investment in Latin American mineral resources and has improved cooperation between geoscience organizations on both continents. The U.S. Geological Survey (USGS) has responded to the new situation through cooperative mineral resource investigations with a number of countries in Latin America. These activities are now being coordinated by the USGS's Center for Inter-American Mineral Resource Investigations (CIMRI), recently established in Tucson, Arizona. In the course of CIMRI's work, we have found a need for a compilation of Spanish geological and mining terminology that goes beyond the few Spanish-English geological dictionaries available. Even geologists who are fluent in Spanish often encounter local terminology oijerga that is unfamiliar. These terms, which have grown out of five centuries of mining tradition in Latin America, and frequently draw on native languages, usually cannot be found in standard dictionaries. There are, of course, many geological terms which can be recognized even by geologists who speak little or no Spanish.